<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Publishing DTD v1.3 20210610//EN" "https://jats.nlm.nih.gov/publishing/1.3/JATS-journalpublishing1-3.dtd"><article xml:lang="en" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:ali="http://www.niso.org/schemas/ali/1.0/" dtd-version="1.3" article-type="other"><front><journal-meta><journal-id journal-id-type="issn">2460-0245</journal-id><journal-title-group><journal-title>Journal of the Indonesian Mathematical Society</journal-title><abbrev-journal-title>JIMS</abbrev-journal-title></journal-title-group><issn pub-type="epub">2460-0245</issn><issn pub-type="ppub">2086-8952</issn><publisher><publisher-name>IndoMS</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.22342/jims.v32i3.1931</article-id><article-categories></article-categories><title-group><article-title>SG-Lightlike Submanifolds of a Locally Bronze Semi-Riemannian Manifold Equipped With (l,m)-Type Connection</article-title></title-group><contrib-group><contrib contrib-type="author"><name><surname>Kaur</surname><given-names>Rajinder</given-names></name><address><country country="IN">India</country><email>rajinderjasar@gmail.com</email></address><xref ref-type="aff" rid="AFF-1"></xref></contrib><contrib contrib-type="author"><name><surname>Kaur</surname><given-names>Jasleen</given-names></name><address><country country="IN">India</country><email>jasleen_math@pbi.ac.in</email></address><xref ref-type="aff" rid="AFF-1"></xref></contrib></contrib-group><contrib-group><contrib contrib-type="editor"><name><surname>Rizal</surname><given-names>Jose</given-names></name><address><email>jrizal04@unib.ac.id</email></address></contrib></contrib-group><aff id="AFF-1"><institution content-type="dept">Department of Mathematics</institution><institution-wrap><institution>Punjabi University</institution><institution-id institution-id-type="ror">https://ror.org/00xdn8y92</institution-id></institution-wrap><country country="IN">India</country></aff><author-notes><fn fn-type="coi-statement"><label>Declarations.</label><p>The authors declare no conflicts of interest.</p></fn></author-notes><pub-date date-type="pub" iso-8601-date="2026-09-01" publication-format="electronic"><day>01</day><month>09</month><year>2026</year></pub-date><pub-date date-type="collection" iso-8601-date="2026-09-01" publication-format="electronic"><day>01</day><month>09</month><year>2026</year></pub-date><volume>32</volume><issue>3</issue><issue-title>Vol. 32 No. 3 (2026): SEPTEMBER</issue-title><fpage>1</fpage><lpage>26</lpage><history><date date-type="received" iso-8601-date="2025-02-02"><day>02</day><month>02</month><year>2025</year></date><date date-type="accepted" iso-8601-date="2026-04-05"><day>05</day><month>04</month><year>2026</year></date></history><permissions><copyright-statement>Copyright (c) 2026 Journal of the Indonesian Mathematical Society</copyright-statement><copyright-year>2026</copyright-year><copyright-holder>Journal of the Indonesian Mathematical Society</copyright-holder><license xlink:href="https://creativecommons.org/licenses/by-nc-nd/4.0/"><ali:license_ref xmlns:ali="http://www.niso.org/schemas/ali/1.0/">https://creativecommons.org/licenses/by-nc-nd/4.0/</ali:license_ref><license-p>This work is licensed under a Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License.</license-p></license></permissions><self-uri xlink:href="https://jims-a.org/index.php/jimsa/article/view/1931" xlink:title="1931"></self-uri><abstract><p>This research work introduces the geometry of the SG (Screen Generic)lightlike submanifolds of a locally bronze semi-Riemannian manifold endowed with an (l,m)-type connection. The characterization theorems on geodesicity of such submanifolds with respect to the integrability and parallelism of the distributions are established. It is shown that there exists no coisotropic, isotropic or totally proper SG-lightlike submanifold of a locally bronze semi-Riemannian manifold. Assertions for the smooth transversal vector fields in totally umbilical proper SG-lightlike submanifold are obtained. Furthermore, the structure of a minimal SG-lightlike submanifold of a locally bronze semi-Riemannian manifold is detailed with an example.</p></abstract><kwd-group><kwd>Locally bronze semi-Riemannian manifold</kwd><kwd>SG-lightlike submanifold</kwd><kwd>Totally umbilical lightlike submanifold</kwd></kwd-group><funding-group><funding-statement>This research received no specific grant from any funding agency in the public, commercial, or not-for-profit sectors.</funding-statement></funding-group><custom-meta-group><custom-meta><meta-name>File created by JATS Editor</meta-name><meta-value>https://jatseditor.com</meta-value></custom-meta><custom-meta><meta-name>issue-created-year</meta-name><meta-value>2026</meta-value></custom-meta></custom-meta-group></article-meta></front><body><sec id="sec-1"><title>1. INTRODUCTION</title><p>De Spinadel <xref ref-type="bibr" rid="BIBR-1">[1]</xref> developed the theory of metallic means family, in which bronze ratio has an important location in studying topics such as dynamical system and quasicrystals. The geometry of bronze structures has an important relation with pure Riemannian metrics according to the corresponding structure. Pandey <xref ref-type="bibr" rid="BIBR-2">[2]</xref> introduced the concept of bronze structure on Riemannian manifold which was further studied by Aknipar <xref ref-type="bibr" rid="BIBR-3">[3]</xref>. Moreover, Duggal and Bejancu <xref ref-type="bibr" rid="BIBR-4">[4]</xref> initiated the theory of lightlike submanifolds of semi-Riemannian manifolds which provides an outstanding framework for geometric characteristics and has versatile applications, particularly in general relativity.</p><p>In view of this, Jin <xref ref-type="bibr" rid="BIBR-5">[5]</xref> developed generic lightlike submanifolds for an indefinite cosymplectic manifold which was further explored by [<xref ref-type="bibr" rid="BIBR-6">6</xref>, <xref ref-type="bibr" rid="BIBR-5">5</xref>] for indefinite Sasakian manifold and indefinite Kaehler manifold, respectively. Several new connections such that semi-symmetric non-metric connection <xref ref-type="bibr" rid="BIBR-7">[7]</xref>, non-metric ϕ- symmetric connection <xref ref-type="bibr" rid="BIBR-8">[8]</xref> etc. applied to the SG-lightlike submanifolds came into existence. <inline-formula><tex-math id="math-1"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \mathrm { A s } \end{document} ]]></tex-math></inline-formula> the generalization of screen Cauchy Riemann(SCR) and generic lightlike submanifolds, Dogan et al. <xref ref-type="bibr" rid="BIBR-9">[9]</xref> introduced the notion of SG-lightlike submanifold for indefinite Kaehler manifold. Then, a few more similar classes namely, contact totally umbilical SG-lightlike and minimal SG-lightlike submanifolds of indefinite Sasakian manifolds were researched by Gupta <xref ref-type="bibr" rid="BIBR-10">[10]</xref>. Recently, the theory of SGlightlike submanifolds was investigated for golden semi-Riemannian manifold <xref ref-type="bibr" rid="BIBR-11">[11]</xref>, cosympletic manifold <xref ref-type="bibr" rid="BIBR-12">[12]</xref> and semi-Riemannian product manifold <xref ref-type="bibr" rid="BIBR-13">[13]</xref>.</p><p>Jin<xref ref-type="bibr" rid="BIBR-14">[14]</xref> introduced the notion of non-symmetric and non-metric <inline-formula><tex-math id="math-2"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula> -type connection on semi-Riemannian manifold as follows: A linear connection Ω on a semi-Riemannian manifold<sup>¯</sup><inline-formula><tex-math id="math-3"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M } ^ { \circ } , \bar { g } ^ { ' } ) \end{document} ]]></tex-math></inline-formula> is called an <inline-formula><tex-math id="math-4"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \ – \end{document} ]]></tex-math></inline-formula> type connection if its torsion tensor <inline-formula><tex-math id="math-5"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { T } ^ { \circ } \end{document} ]]></tex-math></inline-formula> satisfies</p><disp-formula id="equation-1"><tex-math id="math-6"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {T} ^ {\circ} (X ^ {\circ}, Y ^ {\circ}) = l \left\{\theta (Y ^ {\circ}) X ^ {\circ} - \theta (X ^ {\circ}) Y ^ {\circ} \right\} + m \left\{\theta (Y ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} - \theta (X ^ {\circ}) \bar {J} ^ {\prime} Y ^ {\circ} \right\} \end{document} ]]></tex-math></disp-formula><p>where l and m are smooth functions, <inline-formula><tex-math id="math-7"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } ^ { \prime } } \end{document} ]]></tex-math></inline-formula> is a tensor field of <inline-formula><tex-math id="math-8"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( 1 , 1 ) \mathrm { - t y p e } \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-9"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \theta \end{document} ]]></tex-math></inline-formula> is a 1-form associated with a smooth unit spacelike vector field <inline-formula><tex-math id="math-10"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \eta , \end{document} ]]></tex-math></inline-formula> which is called the characteristic vector field, by <inline-formula><tex-math id="math-11"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \theta ( X ^ { \circ } ) = { \bar { g } } ^ { \prime } ( X ^ { \circ } , \eta ) \end{document} ]]></tex-math></inline-formula> . We set <inline-formula><tex-math id="math-12"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \neq ( 0 , 0 ) \end{document} ]]></tex-math></inline-formula> and denote by <inline-formula><tex-math id="math-13"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-14"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle Z ^ { \circ } \end{document} ]]></tex-math></inline-formula> , the smooth vector fields on <inline-formula><tex-math id="math-15"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> . Jin et al. <xref ref-type="bibr" rid="BIBR-15">[15]</xref> further developed the geometry of generic lightlike submanifolds for an indefinite Kaehler manifold equipped with an <inline-formula><tex-math id="math-16"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \mathrm { - t y p e } \end{document} ]]></tex-math></inline-formula> connection. However, the concept of this connection for a locally bronze semi-Riemannian manifold having SG-lightlike submanifolds is yet to be investigated.</p><p>In this paper, we introduce the bronze structure for semi-Riemannian manifold and analyze the geometry of SG-lightlike submanifolds of a locally bronze semi-Riemannian manifolds equipped with an <inline-formula><tex-math id="math-17"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \mathrm { - t y p e } \end{document} ]]></tex-math></inline-formula> connection. The integrability, parallelism and geodesicity of the distributions are characterized. We prove the non-existence of coisotropic, isotropic or totally proper SG-lightlike submanifold of a locally bronze semi-Riemannian manifold. Totally umbilical proper SG-lightlike submanifolds for locally bronze semi-Riemannian manifolds are also worked upon. Additionally, the structure of a minimal SG-lightlike submanifolds has been substantiated with an example.</p></sec><sec id="sec-2"><title>2. PRELIMINARIES</title><p>Let <inline-formula><tex-math id="math-18"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M } ^ { \circ } , \bar { g } ^ { ' } ) \end{document} ]]></tex-math></inline-formula> be an <inline-formula><tex-math id="math-19"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( m + n ) \end{document} ]]></tex-math></inline-formula> -dimensional semi-Riemannian manifold with semi Riemannian metric <inline-formula><tex-math id="math-20"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { g } ^ { \prime } \end{document} ]]></tex-math></inline-formula> of constant index q such that <inline-formula><tex-math id="math-21"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle m , n \geq 1 , 1 \leq q \leq m + n - 1 \end{document} ]]></tex-math></inline-formula> Let <inline-formula><tex-math id="math-22"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( M ^ { \circ } , g ^ { ' } ) \end{document} ]]></tex-math></inline-formula> be an m-dimensional lightlike submanifold of <inline-formula><tex-math id="math-23"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> . There exists a smooth distribution <inline-formula><tex-math id="math-24"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle R a d T M ^ { \circ } \end{document} ]]></tex-math></inline-formula> on <inline-formula><tex-math id="math-25"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> of rank <inline-formula><tex-math id="math-26"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle r > 0 \end{document} ]]></tex-math></inline-formula> , known as radical distribution on <inline-formula><tex-math id="math-27"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> such that RadT <inline-formula><tex-math id="math-28"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ^ { \prime } M _ { p } ^ { \circ } = T M ^ { \circ } { } _ { p } \cap T M ^ { \circ } { } _ { p } ^ { \perp } , \forall p \in M ^ { \circ } \end{document} ]]></tex-math></inline-formula> where <inline-formula><tex-math id="math-29"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M _ { p } ^ { \circ } \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-30"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ \frac { \ d H } { \ d p } } \end{document} ]]></tex-math></inline-formula> are degenerate orthogonal spaces but not complementary. Then <inline-formula><tex-math id="math-31"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is called an r-lightlike submanifold of  <inline-formula><tex-math id="math-32"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ }. \end{document} ]]></tex-math></inline-formula></p><p>Consider complementary distribution of radical distribution in <inline-formula><tex-math id="math-33"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ } \end{document} ]]></tex-math></inline-formula> , called screen distribution, denoted by <inline-formula><tex-math id="math-34"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><inline-formula><tex-math id="math-35"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle i. e. T M ^ {\circ} = R a d T M ^ {\circ} \perp S (T M ^ {\circ}), \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-36"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) \end{document} ]]></tex-math></inline-formula> , called screen transversal vector bundle which is a complementary vector subbundle to <inline-formula><tex-math id="math-37"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle R a d ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> in <inline-formula><tex-math id="math-38"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ _ { - } } \end{document} ]]></tex-math></inline-formula> ⊥</p><disp-formula id="equation-2"><tex-math id="math-39"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ {\circ \perp} = R a d T M ^ {\circ} \perp S (T M ^ {\circ \perp}). \end{document} ]]></tex-math></disp-formula><p>Since S(TM<sup>◦</sup>) is a non degenerate vector subbundle of <inline-formula><tex-math id="math-40"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T \bar { M ^ { \circ } } | _ { M ^ { \circ } } \end{document} ]]></tex-math></inline-formula> , we have</p><disp-formula id="equation-3"><tex-math id="math-41"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \left. T \bar {M} ^ {\circ} \right| _ {M ^ {\circ}} = S (T M ^ {\circ}) \perp S (T M ^ {\circ}) ^ {\perp}, \end{document} ]]></tex-math></disp-formula><p>where <inline-formula><tex-math id="math-42"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) ^ { \perp } \end{document} ]]></tex-math></inline-formula> is the complementary orthogonal vector subbundle of <inline-formula><tex-math id="math-43"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> in <inline-formula><tex-math id="math-44"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T \bar { M ^ { \circ } } | _ { M ^ { \circ } } \end{document} ]]></tex-math></inline-formula></p><p>Let <inline-formula><tex-math id="math-45"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-46"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle l t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> be complementary vector bundles to <inline-formula><tex-math id="math-47"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ } \end{document} ]]></tex-math></inline-formula> in <inline-formula><tex-math id="math-48"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T \bar { M ^ { \circ } } | _ { M ^ { \circ } } \end{document} ]]></tex-math></inline-formula> and to RadTM<sup>◦</sup> in <inline-formula><tex-math id="math-49"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) ^ { \bot } \end{document} ]]></tex-math></inline-formula> . Then</p><disp-formula id="equation-4"><tex-math id="math-50"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & t r (T M ^ {\circ}) = l t r (T M ^ {\circ}) \perp S (T M ^ {\circ^ {\perp}}), \\ & T \bar {M} ^ {\circ} | _ {M ^ {\circ}} = T M ^ {\circ} \oplus t r (T M ^ {\circ}), \\ & \qquad = (R a d T M ^ {\circ} \oplus l t r (T M ^ {\circ})) \perp S (T M ^ {\circ}) \perp S (T M ^ {\circ^ {\perp}}). \end{array} \end{document} ]]></tex-math></disp-formula><p>Following four cases exist for the lightlike submanifold <inline-formula><tex-math id="math-51"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( M ^ { \circ } , g ^ { ' } , S ( T M ^ { \circ } ) , S ( T M ^ { \circ \bot } ) ) \end{document} ]]></tex-math></inline-formula> : </p><p>(1) <inline-formula><tex-math id="math-52"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is r-lightlike if <inline-formula><tex-math id="math-53"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle r < m i n ( m , n ) \end{document} ]]></tex-math></inline-formula></p><p>(2) <inline-formula><tex-math id="math-54"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is co-isotropic i <inline-formula><tex-math id="math-55"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle : r = n < m , { \mathrm { i . e . ~ } } S ( T M ^ { \circ \perp } ) = \{ 0 \} \end{document} ]]></tex-math></inline-formula></p><p>(3) <inline-formula><tex-math id="math-56"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is isotropic if <inline-formula><tex-math id="math-57"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle r = m < n , \mathrm { i . e . } \ S ( T M ^ { \circ } ) = \{ 0 \} \end{document} ]]></tex-math></inline-formula> and</p><p>(4) <inline-formula><tex-math id="math-58"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is totally lightlike if <inline-formula><tex-math id="math-59"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle r = n = m , \mathrm { i . e . } \ S ( T M ^ { \circ \bot } ) = \{ 0 \} = S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula></p><p><bold>Theorem 2.1.</bold><xref ref-type="bibr" rid="BIBR-4">[4]</xref><inline-formula><tex-math id="math-60"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ^ { \prime \prime } L e t \left( M ^ { \circ } , g ^ { ' } , S ( T M ^ { \circ } ) , S ( T M ^ { \circ \bot } ) \right) \end{document} ]]></tex-math></inline-formula><italic> be a r-lightlike submanifold of a semi-Riemannian manifold </italic><inline-formula><tex-math id="math-61"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M } ^ { \circ } , \bar { g } ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> . Then there exists a complementary vector bundle </italic><inline-formula><tex-math id="math-62"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle l t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> , called a lightlike transversal bundle of RadTM</italic><sup><italic>◦</italic></sup><italic> in </italic><inline-formula><tex-math id="math-63"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) ^ { \bot } \end{document} ]]></tex-math></inline-formula><italic> , and a basis of </italic><inline-formula><tex-math id="math-64"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Gamma ( l t r ( T M ^ { \circ } ) | _ { U ^ { \circ } } ) \end{document} ]]></tex-math></inline-formula><italic> consisting of smooth sections </italic><inline-formula><tex-math id="math-65"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ N _ { 1 } ^ { \circ } , \cdots , N _ { r } ^ { \circ } \} \end{document} ]]></tex-math></inline-formula><italic> of </italic><inline-formula><tex-math id="math-66"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) ^ { \bot } | _ { U ^ { \circ } } , \end{document} ]]></tex-math></inline-formula><italic> , where </italic><inline-formula><tex-math id="math-67"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle U ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is a coordinate neighborhood of </italic><inline-formula><tex-math id="math-68"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> , such that</italic></p><disp-formula id="equation-5"><tex-math id="math-69"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {g} ^ {\prime} (N _ {i} ^ {\circ}, \xi_ {j} ^ {\circ}) = \delta_ {i j}, \quad \bar {g} ^ {\prime} (N _ {i} ^ {\circ}, N _ {j} ^ {\circ}) = 0, \quad i, j = 0, 1, \dots , r \end{document} ]]></tex-math></disp-formula><p><italic>where </italic><inline-formula><tex-math id="math-70"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ \xi _ { 1 } ^ { \circ } , \cdots , \xi _ { r } ^ { \circ } \} \end{document} ]]></tex-math></inline-formula><italic> is a lightlike basis of </italic><inline-formula><tex-math id="math-71"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Gamma ( R a d T M ^ { \circ } ) | _ { U ^ { \circ } } . ^ { \prime \prime } \end{document} ]]></tex-math></inline-formula></p><p>Let <inline-formula><tex-math id="math-72"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { \nabla } } ^ { \circ } \end{document} ]]></tex-math></inline-formula> be the Levi-Civita connection on <inline-formula><tex-math id="math-73"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> . Then, the corresponding Gauss and Weingarten formulae are as follows:</p><disp-formula id="equation-6"><tex-math id="math-74"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\nabla} _ {X ^ {\circ}} ^ {\circ} Y ^ {\circ} = \nabla_ {X ^ {\circ}} ^ {\circ} Y ^ {\circ} + h ^ {\circ} (X ^ {\circ}, Y ^ {\circ}), \quad \forall X ^ {\circ}, Y ^ {\circ} \in \Gamma (T M ^ {\circ}),\tag{1} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-7"><tex-math id="math-75"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\nabla} _ {X ^ {\circ}} ^ {\circ} V ^ {\circ} = - A _ {V ^ {\circ}} X ^ {\circ} + \nabla_ {X ^ {\circ}} ^ {\circ^ {t}} V ^ {\circ}, \quad \forall X ^ {\circ} \in \Gamma (T M ^ {\circ}), V ^ {\circ} \in \Gamma (t r (T M ^ {\circ})),\tag{2} \end{document} ]]></tex-math></disp-formula><p>where <inline-formula><tex-math id="math-76"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ \nabla _ { X ^ { \circ } } ^ { \circ } Y ^ { \circ } , A _ { N ^ { \circ } } X ^ { \circ } \} \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-77"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ h ^ { \circ } ( X ^ { \circ } , Y ^ { \circ } ) , \nabla _ { ~ X ^ { \circ } } ^ { \circ t } N ^ { \circ } \} \end{document} ]]></tex-math></inline-formula> belong to <inline-formula><tex-math id="math-78"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-79"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Gamma ( t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula> , respectively. <inline-formula><tex-math id="math-80"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \nabla ^ { \circ } \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-81"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \nabla ^ { \circ ^ { t } } \end{document} ]]></tex-math></inline-formula> are linear connections on <inline-formula><tex-math id="math-82"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> and on the vector bundle tr <inline-formula><tex-math id="math-83"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \cdot ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> , respectively.</p><p>Considering the projection morphisms L and S of <inline-formula><tex-math id="math-84"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> on <inline-formula><tex-math id="math-85"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle l t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-86"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) \end{document} ]]></tex-math></inline-formula> respectively, we have</p><disp-formula id="equation-8"><tex-math id="math-87"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\nabla} _ {X ^ {\circ}} ^ {\circ} Y ^ {\circ} = \nabla_ {X ^ {\circ}} ^ {\circ} Y ^ {\circ} + h ^ {\circ l} (X ^ {\circ}, Y ^ {\circ}) + h ^ {\circ s} (X ^ {\circ}, Y ^ {\circ}),\tag{3} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-9"><tex-math id="math-88"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\nabla} _ {X ^ {\circ}} ^ {\circ} N ^ {\circ} = - A _ {N ^ {\circ}} X ^ {\circ} + \nabla_ {X ^ {\circ}} ^ {\circ l} N ^ {\circ} + D ^ {\circ s} (X ^ {\circ}, N ^ {\circ}),\tag{4} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-10"><tex-math id="math-89"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\nabla} _ {X ^ {\circ}} ^ {\circ} W ^ {\circ} = - A _ {W ^ {\circ}} X ^ {\circ} + \nabla_ {X ^ {\circ}} ^ {\circ s} W ^ {\circ} + D ^ {\circ l} (X ^ {\circ}, W ^ {\circ}),\tag{5} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-11"><tex-math id="math-90"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ {\circ l} \left(X ^ {\circ}, Y ^ {\circ}\right) = L h ^ {\circ} \left(X ^ {\circ}, Y ^ {\circ}\right), h ^ {\circ s} \left(X ^ {\circ}, Y ^ {\circ}\right) = S h ^ {\circ} \left(X ^ {\circ}, Y ^ {\circ}\right), \end{document} ]]></tex-math></disp-formula><p><inline-formula><tex-math id="math-91"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ \nabla ^ { \circ } _ { X ^ { \circ } } Y ^ { \circ } , A _ { N ^ { \circ } } X ^ { \circ } , A _ { W ^ { \circ } } X ^ { \circ } \} \in \Gamma ( T M ^ { \circ } ) , \{ \nabla ^ { \circ l } _ { X ^ { \circ } } N ^ { \circ } , D ^ { \circ l } ( X ^ { \circ } , W ^ { \circ } ) \} \in \Gamma ( l t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-92"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ \nabla ^ { \circ } \ l _ { X ^ { \circ } } ^ { s } W ^ { \circ } , D ^ { \circ { s } } ( X ^ { \circ } , N ^ { \circ } ) \} \in \Gamma ( { \cal S } ( { \cal T } M ^ { \circ \bot } ) ) \end{document} ]]></tex-math></inline-formula> . Then, considering <xref ref-type="disp-formula" rid="equation-8">(3)</xref>-<xref ref-type="disp-formula" rid="equation-10">(5)</xref> and the fact that <inline-formula><tex-math id="math-93"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { \nabla } } ^ { \circ } \end{document} ]]></tex-math></inline-formula> is a metric connection, the following holds:</p><disp-formula id="equation-12"><tex-math id="math-94"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {g} ^ {\prime} (h ^ {\circ s} (X ^ {\circ}, Y ^ {\circ}), W ^ {\circ}) + \bar {g} ^ {\prime} (Y ^ {\circ}, D ^ {\circ l} (X ^ {\circ}, W ^ {\circ})) = \bar {g} ^ {\prime} (A _ {W ^ {\circ}} X ^ {\circ}, Y ^ {\circ}),\tag{6} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-13"><tex-math id="math-95"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {g} ^ {\prime} (D ^ {\circ s} (X ^ {\circ}, N ^ {\circ}), W ^ {\circ}) = \bar {g} ^ {\prime} (A _ {W ^ {\circ}} X ^ {\circ}, N ^ {\circ}).\tag{7} \end{document} ]]></tex-math></disp-formula><p>Let <inline-formula><tex-math id="math-96"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle J ^ { ' } \end{document} ]]></tex-math></inline-formula> be a projection of <inline-formula><tex-math id="math-97"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ } \end{document} ]]></tex-math></inline-formula>on  <inline-formula><tex-math id="math-98"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> . Then, we have</p><disp-formula id="equation-14"><tex-math id="math-99"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \nabla_ {X ^ {\circ}} ^ {\circ} J ^ {'} Y ^ {\circ} = \nabla_ {X ^ {\circ}} ^ {\circ *} J ^ {'} Y ^ {\circ} + h ^ {\circ *} (X ^ {\circ}, J ^ {'} Y ^ {\circ}),\tag{8} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-15"><tex-math id="math-100"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \nabla_ {X ^ {\circ}} ^ {\circ} \xi^ {\circ} = - A _ {\xi^ {\circ}} ^ {*} X ^ {\circ} + \nabla_ {X ^ {\circ}} ^ {* t} \xi^ {\circ},\tag{9} \end{document} ]]></tex-math></disp-formula><p>for any <inline-formula><tex-math id="math-101"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-102"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \xi ^ { \circ } \in \Gamma ( R a d ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula> ), where <inline-formula><tex-math id="math-103"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ \nabla ^ { \circ } { } _ { X ^ { \circ } } ^ { * } J ^ { ' } Y ^ { \circ } , A _ { \xi ^ { \circ } } ^ { * } X ^ { \circ } \} \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-104"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ ( h ^ { \circ * } ( X ^ { \circ } , J ^ { ' } Y ^ { \circ } ) , \nabla ^ { \circ * t } { } _ { X ^ { \circ } } \xi ^ { \circ } \} \end{document} ]]></tex-math></inline-formula> belong to <inline-formula><tex-math id="math-105"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Gamma ( S ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-106"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Gamma ( R a d T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> , respectively. By using the above equations, we obtain</p><disp-formula id="equation-16"><tex-math id="math-107"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {g} ^ {\prime} (h ^ {\circ l} (X ^ {\circ}, J ^ {\prime} Y ^ {\circ}), \xi^ {\circ}) = g ^ {\prime} (A _ {\xi^ {\circ}} ^ {*} X ^ {\circ}, J ^ {\prime} Y ^ {\circ}),\tag{10} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-17"><tex-math id="math-108"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {g} ^ {\prime} (h ^ {\circ *} (X ^ {\circ}, J ^ {\prime} Y ^ {\circ}), N ^ {\circ}) = g ^ {\prime} (A _ {N ^ {\circ}} X ^ {\circ}, J ^ {\prime} Y ^ {\circ}),\tag{11} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-18"><tex-math id="math-109"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {g} ^ {\prime} \left(h ^ {\circ l} \left(X ^ {\circ}, \xi^ {\circ}\right), \xi^ {\circ}\right) = 0, A _ {\xi^ {\circ}} ^ {*} \xi^ {\circ} = 0.\tag{12} \end{document} ]]></tex-math></disp-formula><p>In general, the connection <inline-formula><tex-math id="math-110"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \nabla ^ { \circ } \end{document} ]]></tex-math></inline-formula> on <inline-formula><tex-math id="math-111"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is not metric connection. Since <inline-formula><tex-math id="math-112"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { \nabla } } ^ { \circ } \end{document} ]]></tex-math></inline-formula> is a metric connection, from <xref ref-type="disp-formula" rid="equation-8">(3)</xref>, we derive</p><disp-formula id="equation-19"><tex-math id="math-113"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle (\nabla_ {X ^ {\circ}} ^ {\circ} g ^ {'}) (Y ^ {\circ}, Z ^ {\circ}) = \bar {g} ^ {'} (h ^ {\circ l} (X ^ {\circ}, Y ^ {\circ}), Z ^ {\circ}) + \bar {g} ^ {'} (h ^ {\circ l} (X ^ {\circ}, Z ^ {\circ}), Y ^ {\circ}), \end{document} ]]></tex-math></disp-formula><p>for any <inline-formula><tex-math id="math-114"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } , Z ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> . Here, <inline-formula><tex-math id="math-115"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \nabla ^ { \circ ^ { * } } \end{document} ]]></tex-math></inline-formula> is a metric connection on <inline-formula><tex-math id="math-116"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula></p><p><bold>Definition 2.2.</bold><italic>A polynomial structure on a semi-Riemannian manifold </italic><inline-formula><tex-math id="math-117"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is known as bronze structure if it is determined by </italic><inline-formula><tex-math id="math-118"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } ^ { \prime } } \end{document} ]]></tex-math></inline-formula><italic> such that</italic></p><disp-formula id="equation-20"><tex-math id="math-119"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {J} ^ {2} = 3 \bar {J} ^ {\prime} + I.\tag{13} \end{document} ]]></tex-math></disp-formula><p><italic>where </italic><inline-formula><tex-math id="math-120"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } } ^ { \prime } \end{document} ]]></tex-math></inline-formula><italic> is a tensor field of type (1, 1) on </italic><inline-formula><tex-math id="math-121"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula></p><p><bold>Definition 2.3.</bold><italic>If a semi-Riemannian metric  </italic><inline-formula><tex-math id="math-122"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { g } ^ { \prime } \end{document} ]]></tex-math></inline-formula><italic>satisfies the equation</italic></p><disp-formula id="equation-21"><tex-math id="math-123"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {g} ^ {\prime} (X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}) = \bar {g} ^ {\prime} (\bar {J} ^ {\prime} X ^ {\circ}, Y ^ {\circ}),\tag{14} \end{document} ]]></tex-math></disp-formula><p><italic>which yields</italic></p><disp-formula id="equation-22"><tex-math id="math-124"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {g} ^ {\prime} \left(\bar {J} ^ {\prime} X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}\right) = 3 \bar {g} ^ {\prime} \left(X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}\right) + \bar {g} ^ {\prime} \left(X ^ {\circ}, Y ^ {\circ}\right), \forall X ^ {\circ} Y ^ {\circ} \in \Gamma (T \bar {M} ^ {\circ}),\tag{15} \end{document} ]]></tex-math></disp-formula><p><italic>then </italic><inline-formula><tex-math id="math-125"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { g } ^ { \prime } \end{document} ]]></tex-math></inline-formula><italic> is called </italic><sup><italic>¯</italic></sup><italic>J</italic><sup><italic>′</italic></sup><italic>-compatible.</italic></p><p><bold>Definition 2.4.</bold><italic>”Ifsemi-Riemannian metric </italic><inline-formula><tex-math id="math-126"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { g } ^ { \prime } \end{document} ]]></tex-math></inline-formula><italic> is compatible with the bronze structure </italic><inline-formula><tex-math id="math-127"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } } ^ { \prime } \end{document} ]]></tex-math></inline-formula><italic> , then the pair </italic><inline-formula><tex-math id="math-128"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { g } ^ { \prime } , \bar { J } ^ { \prime } ) \end{document} ]]></tex-math></inline-formula><italic> is called a bronze semi-Riemannian structure and </italic><inline-formula><tex-math id="math-129"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M ^ { \circ } } , \bar { g } ^ { ' } , \bar { J } ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> a bronze semi-Riemannian manifold.”</italic></p><p><bold>Definition 2.5.</bold><inline-formula><tex-math id="math-130"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle I f ( \bar { M ^ { \circ } } , \bar { g } ^ { ' } , \bar { J } ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> is a bronze semi-Riemannian manifold and</italic></p><disp-formula id="equation-23"><tex-math id="math-131"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\nabla} ^ {\circ} \bar {J} ^ {\prime} = 0,\tag{16} \end{document} ]]></tex-math></disp-formula><p><italic>then </italic><inline-formula><tex-math id="math-132"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M ^ { \circ } } , \bar { g } ^ { ' } , \bar { J } ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> is termed as a locally bronze semiRiemannian manifold.</italic></p><p>Let <inline-formula><tex-math id="math-133"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M ^ { \circ } } , \bar { g } ^ { ' } , \bar { J } ^ { ' } ) \end{document} ]]></tex-math></inline-formula> be a locally bronze semi-Riemannian manifold, where <inline-formula><tex-math id="math-134"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { g } ^ { \prime } \end{document} ]]></tex-math></inline-formula> is a semi-Riemannian metric and <inline-formula><tex-math id="math-135"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } } ^ { \prime } \end{document} ]]></tex-math></inline-formula> is a bronze structure. Then, For each <inline-formula><tex-math id="math-136"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \end{document} ]]></tex-math></inline-formula> tangent to <inline-formula><tex-math id="math-137"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } , { \bar { J } } ^ { \prime } X ^ { \circ } \end{document} ]]></tex-math></inline-formula> can be written as follows</p><disp-formula id="equation-24"><tex-math id="math-138"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {J} ^ {\prime} X ^ {\circ} = f ^ {\prime} X ^ {\circ} + w ^ {\prime} X ^ {\circ} = f ^ {\prime} X ^ {\circ} + w _ {l} ^ {\prime} X ^ {\circ} + w _ {s} ^ {\prime} X ^ {\circ},\tag{17} \end{document} ]]></tex-math></disp-formula><p>where <inline-formula><tex-math id="math-139"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle f ^ { ' } X ^ { \circ } \end{document} ]]></tex-math></inline-formula> and w <inline-formula><tex-math id="math-140"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \end{document} ]]></tex-math></inline-formula> are the tangential and the transversal parts of <inline-formula><tex-math id="math-141"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } } ^ { \prime } X ^ { \circ } , w _ { l } ^ { ' } \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-142"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle w _ { s } ^ { ' } \end{document} ]]></tex-math></inline-formula> are the projections on <inline-formula><tex-math id="math-143"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle l t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-144"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) \end{document} ]]></tex-math></inline-formula> ), respectively. In addition, for any <inline-formula><tex-math id="math-145"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle V ^ { \circ } \in \Gamma ( t r ( T M ^ { \circ } ) ) , \bar { J } ^ { \prime } V ^ { \circ } \end{document} ]]></tex-math></inline-formula> can be written as</p><disp-formula id="equation-25"><tex-math id="math-146"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {J} ^ {\prime} V ^ {\circ} = B ^ {\prime} V ^ {\circ} + C ^ {\prime} V ^ {\circ},\tag{18} \end{document} ]]></tex-math></disp-formula><p>where <inline-formula><tex-math id="math-147"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B ^ { ' } V ^ { \circ } \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-148"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle C ^ { ' } V ^ { \circ } \end{document} ]]></tex-math></inline-formula> are the tangential and the transversal parts of <inline-formula><tex-math id="math-149"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } ^ { \prime } } V ^ { \circ } \end{document} ]]></tex-math></inline-formula> , respectively.</p></sec><sec id="sec-3"><title>3. SG-LIGHTLIKE SUBMANIFOLDS</title><p><bold>Definition 3.1.</bold><xref ref-type="bibr" rid="BIBR-9">[9]</xref><italic> A real r-lightlike submanifold M</italic><sup><italic>◦</italic></sup><italic> oflocally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-150"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is said to be a SG-lightlike submanifold of </italic><inline-formula><tex-math id="math-151"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> if the following conditions are satisfied:</italic></p><p><italic>(a) Rad(TM</italic><sup><italic>◦</italic></sup><italic>) is invariant with respect to </italic><inline-formula><tex-math id="math-152"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } } ^ { \prime } \end{document} ]]></tex-math></inline-formula><italic> , that is</italic></p><disp-formula id="equation-26"><tex-math id="math-153"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {J} ^ {\prime} (R a d T M ^ {\circ}) = R a d T M ^ {\circ},\tag{19} \end{document} ]]></tex-math></disp-formula><p><italic>(b) There exist a subbundle </italic><inline-formula><tex-math id="math-154"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } ~ o f ~ S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> such that</italic></p><disp-formula id="equation-27"><tex-math id="math-155"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ {o} = \bar {J} ^ {\prime} (S (T M ^ {\circ})) \cap S (T M ^ {\circ}),\tag{20} \end{document} ]]></tex-math></disp-formula><p><italic>where </italic><inline-formula><tex-math id="math-156"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } \end{document} ]]></tex-math></inline-formula><italic> is a non-degenerate distribution on </italic><inline-formula><tex-math id="math-157"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula></p><p><italic>The above definition implies that there exist a complementary non-degenerate distribution </italic><inline-formula><tex-math id="math-158"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B ^ { ' } \end{document} ]]></tex-math></inline-formula><italic> in </italic><inline-formula><tex-math id="math-159"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> such that</italic></p><disp-formula id="equation-28"><tex-math id="math-160"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S (T M ^ {\circ}) = B _ {o} \oplus B ^ {\prime}, \bar {J} ^ {\prime} (B ^ {\prime}) \not \subseteq S (T M ^ {\circ}), \bar {J} ^ {\prime} (B ^ {\prime}) \not \subseteq S (T M ^ {\circ^ {\perp}}).\tag{21} \end{document} ]]></tex-math></disp-formula><p><italic>Let </italic><inline-formula><tex-math id="math-161"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle J _ { o } , J _ { 1 } \end{document} ]]></tex-math></inline-formula><italic> and Q be the projection morphisms on </italic><inline-formula><tex-math id="math-162"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } , R a d T M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-163"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B ^ { ' } \end{document} ]]></tex-math></inline-formula><italic> respectively. Then for all </italic><inline-formula><tex-math id="math-164"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \in \Gamma ( T M ^ { \circ } ), \end{document} ]]></tex-math></inline-formula></p><disp-formula id="equation-29"><tex-math id="math-165"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ {\circ} = J _ {o} X ^ {\circ} + J _ {1} X ^ {\circ} + Q X ^ {\circ} = J ^ {'} X ^ {\circ} + Q X ^ {\circ}, \end{document} ]]></tex-math></disp-formula><p><italic>where </italic><inline-formula><tex-math id="math-166"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B = B _ { o } \perp R a d T M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> , B is invariant and </italic><inline-formula><tex-math id="math-167"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle J ^ { ' } X ^ { \circ } \in \Gamma ( B ) , Q X ^ { \circ } \in \Gamma ( B ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> It is clear that </italic><inline-formula><tex-math id="math-168"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \boldsymbol { J } } ^ { \prime } ( \boldsymbol { B } ^ { \prime } ) \neq \boldsymbol { B } ^ { \prime } \end{document} ]]></tex-math></inline-formula></p><p><italic>Now for a vector field </italic><inline-formula><tex-math id="math-169"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle Y ^ { \circ } \in \Gamma ( \boldsymbol { B } ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> and using </italic><xref ref-type="disp-formula" rid="equation-24">(17)</xref><italic>, we have</italic></p><disp-formula id="equation-30"><tex-math id="math-170"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {J} ^ {\prime} Y ^ {\circ} = f ^ {\prime} Y ^ {\circ} + w ^ {\prime} Y ^ {\circ},\tag{22} \end{document} ]]></tex-math></disp-formula><p><italic>where </italic><inline-formula><tex-math id="math-171"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle f ^ { ' } Y ^ { \circ } \in \Gamma ( B ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> and w </italic><inline-formula><tex-math id="math-172"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle Y ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \bot } ) ) \end{document} ]]></tex-math></inline-formula><italic> ).</italic></p><p><inline-formula><tex-math id="math-173"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is said to be a proper SG-lightlike submanifold of a locally bronze semi-Riemannian manifold if </italic><inline-formula><tex-math id="math-174"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } \neq \{ 0 \} \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-175"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B ^ { ' } \neq \{ 0 \} \end{document} ]]></tex-math></inline-formula></p><p><italic>Proposition 3.2. Let </italic><inline-formula><tex-math id="math-176"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> be an SG-lightlike submanifold of a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-177"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M } ^ { \circ } , \bar { g } ^ { ' } , \bar { J } ^ { \prime } ) \end{document} ]]></tex-math></inline-formula><italic> . Then, the distribution </italic><inline-formula><tex-math id="math-178"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle l t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> is invariant with respect to </italic><inline-formula><tex-math id="math-179"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } } ^ { \prime } \end{document} ]]></tex-math></inline-formula></p></sec><sec id="sec-4"><title>4. (l, m)-TYPE CONNECTION</title><p>For Levi-Civita connection <inline-formula><tex-math id="math-180"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { \nabla } } ^ { \circ } \end{document} ]]></tex-math></inline-formula> on the locally bronze semi-Riemannian manifold <inline-formula><tex-math id="math-181"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M } ^ { \circ } , \bar { g } ^ { ' } , \bar { J } ^ { ' } ) \end{document} ]]></tex-math></inline-formula> , we set</p><disp-formula id="equation-31"><tex-math id="math-182"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\Omega} _ {X ^ {\circ}} Y ^ {\circ} = \bar {\nabla} _ {X ^ {\circ}} ^ {\circ} Y ^ {\circ} + \theta (Y ^ {\circ}) \{l X ^ {\circ} + m \bar {J} ^ {\prime} X ^ {\circ} \},\tag{23} \end{document} ]]></tex-math></disp-formula><p>for any <inline-formula><tex-math id="math-183"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> . Since <inline-formula><tex-math id="math-184"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { \nabla } } ^ { \circ } \end{document} ]]></tex-math></inline-formula> is torsion free and metric connection, therefore we obtain</p><disp-formula id="equation-32"><tex-math id="math-185"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {(\bar {\Omega} _ {X ^ {\circ}} \bar {g} ^ {'}) (Y ^ {\circ}, Z ^ {\circ}) = - l \{\theta (Y ^ {\circ}) \bar {g} ^ {'} (X ^ {\circ}, Z ^ {\circ}) + \theta (Z ^ {\circ}) \bar {g} ^ {'} (X ^ {\circ}, Y ^ {\circ}) \}} \\ & {- m \theta (Y ^ {\circ}) \bar {g} ^ {'} (\bar {J} ^ {'} X ^ {\circ}, Z ^ {\circ}) - m \theta (Z ^ {\circ}) \bar {g} ^ {'} (\bar {J} ^ {'} X ^ {\circ}, Y ^ {\circ}),} \end{array}\tag{24} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-33"><tex-math id="math-186"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {T} ^ {\circ} (X ^ {\circ}, Y ^ {\circ}) = l \{\theta (Y ^ {\circ}) X ^ {\circ} - \theta (X ^ {\circ}) Y ^ {\circ} \} + m \{\theta (Y ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} - \theta (X ^ {\circ}) \bar {J} ^ {\prime} Y ^ {\circ} \}, \end{document} ]]></tex-math></disp-formula><p>for any <inline-formula><tex-math id="math-187"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } , Z ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> , where <inline-formula><tex-math id="math-188"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { T ^ { \circ } } ^ { \bar { \Omega } } \end{document} ]]></tex-math></inline-formula> is a torsion tensor of the connection <inline-formula><tex-math id="math-189"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } . \end{document} ]]></tex-math></inline-formula> where l and m are smooth functions and θ is a 1-form associated with a smooth unit spacelike vector field <inline-formula><tex-math id="math-190"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \eta , \end{document} ]]></tex-math></inline-formula> termed as the characteristic vector field, by <inline-formula><tex-math id="math-191"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \theta ( X ^ { \circ } ) = \end{document} ]]></tex-math></inline-formula><inline-formula><tex-math id="math-192"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { g } ^ { \prime } ( X ^ { \circ } , \eta ) \end{document} ]]></tex-math></inline-formula> . Setting <inline-formula><tex-math id="math-193"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \neq ( 0 , 0 ) \end{document} ]]></tex-math></inline-formula> , Ω is called an<sup>¯</sup><inline-formula><tex-math id="math-194"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula> -type connection. Since <inline-formula><tex-math id="math-195"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> admits a tensor field <inline-formula><tex-math id="math-196"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } ^ { \prime } } \end{document} ]]></tex-math></inline-formula> of type (1, 1), therefore for any <inline-formula><tex-math id="math-197"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> , we have</p><disp-formula id="equation-34"><tex-math id="math-198"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{c} (\bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {\prime}) (Y ^ {\circ}) = l \{\theta (\bar {J} ^ {\prime} Y ^ {\circ}) X ^ {\circ} - \theta (Y ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} \} + m \{\theta (\bar {J} ^ {\prime} Y ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} \\ - 3 \theta (Y ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} - \theta (Y ^ {\circ}) X ^ {\circ} \}, \end{array} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-35"><tex-math id="math-199"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{c} \bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ} = \bar {J} ^ {\prime} (\bar {\Omega} _ {X ^ {\circ}} Y ^ {\circ}) + l \{\theta (\bar {J} ^ {\prime} Y ^ {\circ}) X ^ {\circ} - \theta (Y ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} \} + m \{\theta (\bar {J} ^ {\prime} Y ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} \\ - 3 \theta (Y ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} - \theta (Y ^ {\circ}) X ^ {\circ} \}. \end{array}\tag{25} \end{document} ]]></tex-math></disp-formula><p>Let <inline-formula><tex-math id="math-200"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( M ^ { \circ } , g ^ { ' } , S ( T M ^ { \circ } ) , S ( T M ^ { \circ \bot } ) ) \end{document} ]]></tex-math></inline-formula> be a SG-lightlike submanifold of a locally bronze semi-Riemannian manifold <inline-formula><tex-math id="math-201"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M } ^ { \circ } , \bar { g } ^ { ' } ) \end{document} ]]></tex-math></inline-formula> with an <inline-formula><tex-math id="math-202"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula> type connection Ω. Let Ω be the<sup>¯</sup> induced linear connection on <inline-formula><tex-math id="math-203"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> from Ω. Therefore the Gauss formula inherent in<sup>¯</sup> its structure is as follows:</p><disp-formula id="equation-36"><tex-math id="math-204"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\Omega} _ {X ^ {\circ}} Y ^ {\circ} = \Omega_ {X ^ {\circ}} Y ^ {\circ} + \bar {h ^ {\circ}} ^ {l} (X ^ {\circ}, Y ^ {\circ}) + \bar {h ^ {\circ}} ^ {s} (X ^ {\circ}, Y ^ {\circ}),\tag{26} \end{document} ]]></tex-math></disp-formula><p>for any <inline-formula><tex-math id="math-205"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> , where <inline-formula><tex-math id="math-206"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Omega _ { X ^ { \circ } } Y ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> , and <inline-formula><tex-math id="math-207"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { h ^ { \circ } } ^ { l } , \bar { h ^ { \circ } } ^ { s } \end{document} ]]></tex-math></inline-formula> are lightlike second fundamental form and the screen second fundamental form of <inline-formula><tex-math id="math-208"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> , respectively. Now from <xref ref-type="disp-formula" rid="equation-8">(3)</xref>, <xref ref-type="disp-formula" rid="equation-24">(17)</xref>, <xref ref-type="disp-formula" rid="equation-31">(23)</xref> and <xref ref-type="disp-formula" rid="equation-36">(26)</xref>, we obtain</p><disp-formula id="equation-37"><tex-math id="math-209"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Omega_ {X ^ {\circ}} Y ^ {\circ} = \nabla_ {X ^ {\circ}} ^ {\circ} Y ^ {\circ} + l \theta (Y ^ {\circ}) X ^ {\circ} + m \theta (Y ^ {\circ}) f ^ {'} X ^ {\circ},\tag{27} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-38"><tex-math id="math-210"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {h ^ {\circ}} ^ {l} (X ^ {\circ}, Y ^ {\circ}) = h ^ {\circ l} (X ^ {\circ}, Y ^ {\circ}) + m \theta (Y ^ {\circ}) w _ {l} ^ {'} X ^ {\circ},\tag{28} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-39"><tex-math id="math-211"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {h ^ {\circ}} ^ {s} (X ^ {\circ}, Y ^ {\circ}) = h ^ {\circ s} (X ^ {\circ}, Y ^ {\circ}) + m \theta (Y ^ {\circ}) w _ {s} ^ {'} X ^ {\circ},\tag{29} \end{document} ]]></tex-math></disp-formula><p>Moreover using, <xref ref-type="disp-formula" rid="equation-24">(17)</xref>, <xref ref-type="disp-formula" rid="equation-30">(22)</xref>, <xref ref-type="disp-formula" rid="equation-32">(24)</xref> and <xref ref-type="disp-formula" rid="equation-36">(26)</xref>, we get,</p><disp-formula id="equation-40"><tex-math id="math-212"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{c} (\Omega_ {X ^ {\circ}} g ^ {'}) (Y ^ {\circ}, Z ^ {\circ}) = g ^ {'} (h ^ {\circ l} (X ^ {\circ}, Y ^ {\circ}), Z ^ {\circ}) + g ^ {'} (Y ^ {\circ}, h ^ {\circ l} (X ^ {\circ}, Z ^ {\circ})) \\ - l (\theta (Y ^ {\circ}) g ^ {'} (X ^ {\circ}, Z ^ {\circ}) + \theta (Z ^ {\circ}) g ^ {'} (Y ^ {\circ}, X ^ {\circ})) \\ - m (\theta (Y ^ {\circ}) g ^ {'} (f ^ {'} X ^ {\circ}, Z ^ {\circ}) + \theta (Z ^ {\circ}) g ^ {'} (Y ^ {\circ}, f ^ {'} Z ^ {\circ})), \end{array}\tag{30} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-41"><tex-math id="math-213"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T ^ {\circ \Omega} (X ^ {\circ}, Y ^ {\circ}) = l \{\theta (Y ^ {\circ}) X ^ {\circ} - \theta (X ^ {\circ}) Y ^ {\circ} \} + m \{\theta (Y ^ {\circ}) f ^ {^ {\prime}} X ^ {\circ} - \theta (X ^ {\circ}) f ^ {^ {\prime}} Y ^ {\circ} \}, \end{document} ]]></tex-math></disp-formula><p>for any <inline-formula><tex-math id="math-214"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } , Z ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> , where <inline-formula><tex-math id="math-215"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T ^ { \circ \Omega } \end{document} ]]></tex-math></inline-formula> is torsion tensor of the induced connection Ω on <inline-formula><tex-math id="math-216"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> . Hence, the following result holds:</p><p>Theorem 4.1. The induced connection Ω on the SG-lightlike submanifold <inline-formula><tex-math id="math-217"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> of a locally bronze semi-Riemannian manifold <inline-formula><tex-math id="math-218"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> with an <inline-formula><tex-math id="math-219"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula> -type connection Ω<sup>¯</sup>, <inline-formula><tex-math id="math-220"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } \end{document} ]]></tex-math></inline-formula> is also an (l, m)-type connection.</p><p>Suppose that <inline-formula><tex-math id="math-221"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { h ^ { \circ } } ^ { l } \end{document} ]]></tex-math></inline-formula> vanishes identically on <inline-formula><tex-math id="math-222"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> . Therefore</p><disp-formula id="equation-42"><tex-math id="math-223"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {(\Omega_ {X ^ {\circ}} g ^ {'}) (Y ^ {\circ}, Z ^ {\circ}) = - l (\theta (Y ^ {\circ}) g ^ {'} (X ^ {\circ}, Z ^ {\circ}) + \theta (Z ^ {\circ}) g ^ {'} (Y ^ {\circ}, X ^ {\circ}))} \\ & {- m (\theta (Y ^ {\circ}) g ^ {'} (f ^ {'} X ^ {\circ}, Z ^ {\circ}) + \theta (Z ^ {\circ}) g ^ {'} (Y ^ {\circ}, f ^ {'} Z ^ {\circ})),} \end{array}\tag{31} \end{document} ]]></tex-math></disp-formula><p>follows from <xref ref-type="disp-formula" rid="equation-40">(30)</xref>.</p><p>Consequently, we attain the following result:</p><p><bold>Theorem 4.2.</bold><italic>For a SG-lightlike submanifold </italic><inline-formula><tex-math id="math-224"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> ofa locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-225"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> with an </italic><inline-formula><tex-math id="math-226"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula><italic> -type connection </italic><inline-formula><tex-math id="math-227"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } \end{document} ]]></tex-math></inline-formula><italic> , the induced connection Ω on </italic><inline-formula><tex-math id="math-228"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is also an (l, m)-type connection if and only </italic><inline-formula><tex-math id="math-229"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle i f \bar { h ^ { \circ } } ^ { l } \end{document} ]]></tex-math></inline-formula><italic> vanishes identically on </italic><inline-formula><tex-math id="math-230"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> and the characterstic vector field </italic><inline-formula><tex-math id="math-231"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \zeta \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula><italic> such that </italic><inline-formula><tex-math id="math-232"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \theta ( X ^ { \circ } ) = { \bar { g } } ^ { \prime } ( X ^ { \circ } , \zeta ). \end{document} ]]></tex-math></inline-formula></p><p>Corresponding to an <inline-formula><tex-math id="math-233"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) { \mathrm { - t y } } \end{document} ]]></tex-math></inline-formula> pe connection Ω, the Weingarten formulae are<sup>¯</sup> given by:</p><disp-formula id="equation-43"><tex-math id="math-234"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\Omega} _ {X ^ {\circ}} N ^ {\circ} = - \bar {A} _ {N ^ {\circ}} X ^ {\circ} + \bar {\Omega} _ {X ^ {\circ}} ^ {l} N ^ {\circ} + \bar {D} ^ {\circ^ {s}} (X ^ {\circ}, N ^ {\circ}),\tag{32} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-44"><tex-math id="math-235"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\Omega} _ {X ^ {\circ}} W ^ {\circ} = - \bar {A} _ {W ^ {\circ}} X ^ {\circ} + \bar {\Omega} _ {X ^ {\circ}} ^ {s} W ^ {\circ} + \bar {D} ^ {\circ^ {l}} (X ^ {\circ}, W ^ {\circ}),\tag{33} \end{document} ]]></tex-math></disp-formula><p><inline-formula><tex-math id="math-236"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle N ^ { \circ } \in \Gamma ( l t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-237"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula> , where <inline-formula><tex-math id="math-238"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ \bar { A } _ { N ^ { \circ } } X ^ { \circ } , \bar { A } _ { W ^ { \circ } } X ^ { \circ } \} \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> 2 <inline-formula><tex-math id="math-239"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ \bar { \Omega } _ { X ^ { \circ } } ^ { l } N ^ { \circ } , \bar { D ^ { \circ } } { } ^ { l } ( X ^ { \circ } , W ^ { \circ } ) \} \in \Gamma ( l t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-240"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ \bar { \Omega } _ { X ^ { \circ } } ^ { s } W ^ { \circ } , \bar { D ^ { \circ } } ^ { s } ( X ^ { \circ } , N ^ { \circ } ) \} \in \Gamma ( S ( T M ^ { \circ \bot } ) ) \end{document} ]]></tex-math></inline-formula><inline-formula><tex-math id="math-241"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } ^ { l } \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-242"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } ^ { s } \end{document} ]]></tex-math></inline-formula> are linear connections on <inline-formula><tex-math id="math-243"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle l t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-244"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) \end{document} ]]></tex-math></inline-formula> , respectively. Both <inline-formula><tex-math id="math-245"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { A } _ { N ^ { \circ } } \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-246"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { A } _ { W ^ { \circ } } \end{document} ]]></tex-math></inline-formula> are linear operators on <inline-formula><tex-math id="math-247"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Gamma ( T M ^ { \circ } ). \end{document} ]]></tex-math></inline-formula></p><p>Now, employing equations <xref ref-type="disp-formula" rid="equation-9">(4)</xref>, <xref ref-type="disp-formula" rid="equation-10">(5)</xref>, <xref ref-type="disp-formula" rid="equation-31">(23)</xref>, <xref ref-type="disp-formula" rid="equation-43">(32)</xref> and <xref ref-type="disp-formula" rid="equation-44">(33)</xref>, we attain</p><disp-formula id="equation-45"><tex-math id="math-248"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {A} _ {N ^ {\circ}} X ^ {\circ} = A _ {N ^ {\circ}} X ^ {\circ} - l \theta (N ^ {\circ}) X ^ {\circ} - m \theta (N ^ {\circ}) f ^ {'} X ^ {\circ},\tag{34} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-46"><tex-math id="math-249"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}\bar{\Omega}^{l}_{X^\circ} N^\circ &= \nabla^{l}_{X^\circ} N^\circ + m\theta(N^\circ) w'_l X^\circ, \\\bar{D}^{\circ s}(X^\circ, N^\circ) &= D^{\circ s}(X^\circ, N^\circ) + m\theta(N^\circ) w'_s X^\circ,\end{align*}\tag{35} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-47"><tex-math id="math-250"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {A} _ {W ^ {\circ}} X ^ {\circ} = A _ {W ^ {\circ}} X ^ {\circ} - l \theta (W ^ {\circ}) X ^ {\circ} - m \theta (W ^ {\circ}) f ^ {'} X ^ {\circ},\tag{36} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-48"><tex-math id="math-251"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}\bar{\Omega}^{s}_{X^\circ} W^\circ &= \nabla^{s}_{X^\circ} W^\circ + m\theta(W^\circ) w'_s X^\circ, \\\bar{D}^{\circ l}(X^\circ, W^\circ) &= D^{\circ l}(X^\circ, W^\circ) + m\theta(W^\circ) w'_l X^\circ,\end{align*}\tag{37} \end{document} ]]></tex-math></disp-formula><p>Now, using equations <xref ref-type="disp-formula" rid="equation-12">(6)</xref>, <xref ref-type="disp-formula" rid="equation-13">(7)</xref>, <xref ref-type="disp-formula" rid="equation-39">(29)</xref>, <xref ref-type="disp-formula" rid="equation-46">(35)</xref> and <xref ref-type="disp-formula" rid="equation-48">(37),</xref> we obtain</p><disp-formula id="equation-49"><tex-math id="math-252"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {g} ^ {\prime} (\bar {h} ^ {\circ s} (X ^ {\circ}, Y ^ {\circ}), W ^ {\circ}) + \bar {g} ^ {\prime} (Y ^ {\circ}, \bar {D} ^ {\circ l} (X ^ {\circ}, W ^ {\circ})) = \bar {g} ^ {\prime} (\bar {A} _ {W ^ {\circ}} X ^ {\circ}, Y ^ {\circ}) \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-50"><tex-math id="math-253"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle + l \theta (W ^ {\circ}) \bar {g} ^ {\prime} (X ^ {\circ}, Y ^ {\circ}) + m \theta (W ^ {\circ}) \bar {g} ^ {\prime} (f ^ {\prime} X ^ {\circ}, Y ^ {\circ})\tag{38} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-51"><tex-math id="math-254"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle + m \theta (Y ^ {\circ}) \bar {g} ^ {\prime} (w _ {s} ^ {\prime} X ^ {\circ}, W ^ {\circ}) + m \theta (W ^ {\circ}) \bar {g} ^ {\prime} (X ^ {\circ}, w _ {l} ^ {\prime} X ^ {\circ}), \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-52"><tex-math id="math-255"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {\bar {g} ^ {'} (\bar {D} ^ {\circ^ {s}} (X ^ {\circ}, N ^ {\circ}), W ^ {\circ}) = \bar {g} ^ {'} (\bar {A} _ {W ^ {\circ}} X ^ {\circ}, N ^ {\circ}) + l \theta (W ^ {\circ}) \bar {g} ^ {'} (X ^ {\circ}, N ^ {\circ})} \\ & {\qquad + m \theta (W ^ {\circ}) \bar {g} ^ {'} (f ^ {'} X ^ {\circ}, N ^ {\circ}) + m \theta (N ^ {\circ}) \bar {g} ^ {'} (w _ {s} ^ {'} X ^ {\circ}, W ^ {\circ}),} \end{array} \end{document} ]]></tex-math></disp-formula><p>Let  <inline-formula><tex-math id="math-256"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle J ^ { ' } \end{document} ]]></tex-math></inline-formula> be the projection of <inline-formula><tex-math id="math-257"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ } \end{document} ]]></tex-math></inline-formula> on <inline-formula><tex-math id="math-258"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> , then any <inline-formula><tex-math id="math-259"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> can be written as <inline-formula><tex-math id="math-260"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } = J ^ { ' } X ^ { \circ } + \Sigma _ { i = 1 } ^ { r } \eta _ { i } ( X ^ { \circ } ) \xi _ { i } ^ { \circ } \end{document} ]]></tex-math></inline-formula> 2 <inline-formula><tex-math id="math-261"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \eta_ {i} (X ^ {\circ}) = g (X ^ {\circ}, N _ {i} ^ {\circ}), \end{document} ]]></tex-math></inline-formula> where <inline-formula><tex-math id="math-262"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ \xi _ { i } ^ { \circ } \} _ { i = 1 } ^ { r } \end{document} ]]></tex-math></inline-formula> is a basis for Rad <inline-formula><tex-math id="math-263"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ } \end{document} ]]></tex-math></inline-formula> . The subsequent decomposition w.r.t Ω is</p><disp-formula id="equation-53"><tex-math id="math-264"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Omega_ {X ^ {\circ}} J ^ {'} Y ^ {\circ} = \Omega_ {X ^ {\circ}} ^ {*} J ^ {'} Y ^ {\circ} + \bar {h ^ {\circ}} ^ {*} (X ^ {\circ}, J ^ {'} Y ^ {\circ}),\tag{39} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-54"><tex-math id="math-265"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Omega_ {X ^ {\circ}} \xi^ {\circ} = - \bar {A} _ {\xi^ {\circ}} ^ {*} X ^ {\circ} + \bar {\Omega} _ {X ^ {\circ}} ^ {* t} \xi^ {\circ},\tag{40} \end{document} ]]></tex-math></disp-formula><p>for any <inline-formula><tex-math id="math-266"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> , where <inline-formula><tex-math id="math-267"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ \Omega _ { X ^ { \circ } } ^ { \ast } J ^ { ' } Y ^ { \circ } , \bar { A } _ { \xi ^ { \circ } } ^ { \ast } X ^ { \circ } \} \in \Gamma ( S ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula> and {h<sup>¯◦∗</sup>(X<sup>◦</sup>, J<sup>′</sup>Y<sup>◦</sup>), Ω<sup>¯</sup><sup>∗t</sup>◦ξ<sup>◦</sup>} ∈ Γ(RadTM<sup>◦</sup>).</p><p>From <xref ref-type="disp-formula" rid="equation-14">(8)</xref>, <xref ref-type="disp-formula" rid="equation-15">(9)</xref>, <xref ref-type="disp-formula" rid="equation-24">(17)</xref>, <xref ref-type="disp-formula" rid="equation-53">(39)</xref> and <xref ref-type="disp-formula" rid="equation-54">(40)</xref>, we obtain</p><disp-formula id="equation-55"><tex-math id="math-268"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Omega_ {X ^ {\circ}} ^ {*} J ^ {'} Y ^ {\circ} = \nabla_ {X ^ {\circ}} ^ {\circ *} J ^ {'} Y ^ {\circ} + m \theta (J ^ {'} Y ^ {\circ}) J ^ {'} f ^ {'} X ^ {\circ} + l \theta (J ^ {'} Y ^ {\circ}) J ^ {'} X ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-56"><tex-math id="math-269"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r} \bar {h} ^ {\circ *} (X ^ {\circ}, J ^ {'} Y ^ {\circ}) = h ^ {\circ *} (X ^ {\circ}, J ^ {'} Y ^ {\circ}) + l \theta (J ^ {'} Y ^ {\circ}) \Sigma_ {i = 1} ^ {r} \eta_ {i} (X ^ {\circ}) \xi_ {i} ^ {\circ} \\ + m \theta (J ^ {'} Y ^ {\circ}) \Sigma_ {i = 1} ^ {r} \eta_ {i} (f ^ {'} X ^ {\circ}) \xi_ {i} ^ {\circ}, \end{array}\tag{41} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-57"><tex-math id="math-270"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {A} _ {\xi^ {\circ}} ^ {*} X ^ {\circ} = A _ {\xi^ {\circ}} ^ {*} X ^ {\circ} - l \theta (\xi^ {\circ}) J ^ {\prime} X ^ {\circ} - m \theta (\xi^ {\circ}) J ^ {\prime} f ^ {\prime} X ^ {\circ},\tag{42} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-58"><tex-math id="math-271"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\Omega} _ {X ^ {\circ}} ^ {* t} \xi^ {\circ} = \nabla_ {X ^ {\circ}} ^ {\circ * t} \xi^ {\circ} + l \theta (\xi^ {\circ}) \eta (X ^ {\circ}) \xi^ {\circ} + m \theta (\xi^ {\circ}) \eta (f ^ {'} X ^ {\circ}) \xi^ {\circ}, \end{document} ]]></tex-math></disp-formula><p>Further, using <xref ref-type="disp-formula" rid="equation-16">(10)</xref>, <xref ref-type="disp-formula" rid="equation-17">(11)</xref>, <xref ref-type="disp-formula" rid="equation-18">(12)</xref>, <xref ref-type="disp-formula" rid="equation-56">(41)</xref> and <xref ref-type="disp-formula" rid="equation-57">(42)</xref>, we derive</p><disp-formula id="equation-59"><tex-math id="math-272"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r} g ^ {'} (\bar {h} ^ {\circ l} (X ^ {\circ}, J ^ {'} Y ^ {\circ}), \xi^ {\circ}) = g ^ {'} (\bar {A} _ {\xi^ {\circ}} ^ {*} X ^ {\circ}, J ^ {'} Y ^ {\circ}) + l \theta (\xi^ {\circ}) g ^ {'} (J ^ {'} X ^ {\circ}, J ^ {'} Y ^ {\circ}) + \\ m \theta (\xi^ {\circ}) g ^ {'} (J ^ {'} f ^ {'} X ^ {\circ}, J ^ {'} Y ^ {\circ}) + m \theta (J ^ {'} Y ^ {\circ}) g ^ {'} (w _ {l} ^ {'} X ^ {\circ}, \xi^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-60"><tex-math id="math-273"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & g ^ {'} (\bar {h ^ {\circ}} ^ {*} (X ^ {\circ}, J ^ {'} Y ^ {\circ}), N ^ {\circ}) = g ^ {'} (\bar {A} _ {N ^ {\circ}} X ^ {\circ}, J ^ {'} Y ^ {\circ}) + l \theta (N ^ {\circ}) g ^ {'} (X ^ {\circ}, J ^ {'} Y ^ {\circ}) \\ & \qquad + m \theta (N ^ {\circ}) g ^ {'} (f ^ {'} X ^ {\circ}, J ^ {'} Y ^ {\circ}) + m \theta (J ^ {'} Y ^ {\circ}) \eta (f ^ {'} X ^ {\circ}), \\ & \qquad g ^ {'} (\bar {h ^ {\circ}} ^ {l} (X ^ {\circ}, \xi^ {\circ}), \xi^ {\circ}) = m \theta (\xi^ {\circ}) g ^ {'} (w _ {l} ^ {'} X ^ {\circ}, \xi^ {\circ}), \\ & \qquad \bar {A} _ {\xi^ {\circ}} ^ {*} \xi^ {\circ} = - l \theta (\xi^ {\circ}) J ^ {'} \xi^ {\circ} - m \theta (\xi^ {\circ}) J ^ {'} f ^ {'} \xi^ {\circ}, \end{array} \end{document} ]]></tex-math></disp-formula></sec><sec id="sec-5"><title>5. SG-LIGHTLIKE SUBMANIFOLDS WITH AN (l,m)-TYPE CONNECTION</title><p><bold>Definition 5.1.</bold><italic>"Let </italic><inline-formula><tex-math id="math-274"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> be a lightlike submanifold of a locally bronze semi-Riemannian manifold  </italic><inline-formula><tex-math id="math-275"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> . If</italic></p><disp-formula id="equation-61"><tex-math id="math-276"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {J} ^ {\prime} \operatorname{Rad} (T M ^ {\circ}) = \operatorname{Rad} (T M ^ {\circ}), \quad \bar {J} ^ {\prime} S (T M ^ {\circ}) = S (T M ^ {\circ}),\tag{43} \end{document} ]]></tex-math></disp-formula><p><italic>then </italic><inline-formula><tex-math id="math-277"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is an invariant lightlike submanifold of a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-278"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula></p><p><bold>Proposition 5.2.</bold><italic> A screen Cauchy Riemann (SCR) lightlike submanifold of a locally bronze semi-Riemannian manifold is a SG-lightlike submanifold such that distribution B is totally anti-invariant , that is,</italic></p><disp-formula id="equation-62"><tex-math id="math-279"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S (TM^{\circ^ {\perp}}) = \omega^ {\prime} B ^ {\prime} \oplus \mu^ {\circ},\tag{44} \end{document} ]]></tex-math></disp-formula><p><italic>where </italic><inline-formula><tex-math id="math-280"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \omega ^ { ' } \end{document} ]]></tex-math></inline-formula><italic> is the normal component of bronze semi-Riemannian structure and </italic><inline-formula><tex-math id="math-281"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \mu ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is a non-degenerate invariant distribution.</italic></p><p><bold>Proposition 5.3.</bold><italic>There is a non-existence of coisotropic , isotropic or totally proper SG-lightlike submanifold </italic><inline-formula><tex-math id="math-282"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> of a locally bronze semi-Riemannian manifold. If M</italic><sup><italic>◦</italic></sup><italic> is SG-isotropic, coisotropic or totally lightlike submanifold, then it is invariant lightlike submanifold.</italic></p><p><italic>Proof</italic>. Let <inline-formula><tex-math id="math-283"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> be a proper SG-lightlike submanifold of a locally bronze semi-Riemannian manifold <inline-formula><tex-math id="math-284"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> . Let <inline-formula><tex-math id="math-285"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is isotropic, <inline-formula><tex-math id="math-286"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) = \{ 0 \} \end{document} ]]></tex-math></inline-formula> which implies that <inline-formula><tex-math id="math-287"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } = \{ 0 \} \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-288"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B ^ { ' } = \{ 0 \} \end{document} ]]></tex-math></inline-formula> Therefore, <inline-formula><tex-math id="math-289"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } R a d ( T M ^ { \circ } ) = R a d ( T M ^ { \circ } ). \end{document} ]]></tex-math></inline-formula> Hence, <inline-formula><tex-math id="math-290"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ } = R a d ( T M ^ { \circ } ) = \bar { J } ^ { \prime } R a d ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> which shows that <inline-formula><tex-math id="math-291"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is invariant submanifold with respect to <inline-formula><tex-math id="math-292"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } } ^ { \prime } \end{document} ]]></tex-math></inline-formula> . If <inline-formula><tex-math id="math-293"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is coisotropic, then <inline-formula><tex-math id="math-294"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) = \{ 0 \} \end{document} ]]></tex-math></inline-formula> . Therefore, using <xref ref-type="disp-formula" rid="equation-62">(44)</xref>, we obtain <inline-formula><tex-math id="math-295"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \mu ^ { \circ } = 0 \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-296"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } ( B ^ { ' } ) = 0 \end{document} ]]></tex-math></inline-formula> . Also, <inline-formula><tex-math id="math-297"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ } = B _ { o } \oplus \bar { J } ^ { \prime } ( B ^ { ' } ) \end{document} ]]></tex-math></inline-formula> ⊕ <inline-formula><tex-math id="math-298"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle R a d ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-299"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is invariant with respect to <inline-formula><tex-math id="math-300"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } ^ { \prime } } \end{document} ]]></tex-math></inline-formula> . Further, if <inline-formula><tex-math id="math-301"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is totally lightlike, then <inline-formula><tex-math id="math-302"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) = \{ 0 \} \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-303"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) = \{ 0 \} \end{document} ]]></tex-math></inline-formula> . Thus, we obtain <inline-formula><tex-math id="math-304"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ } = R a d ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> which proves <inline-formula><tex-math id="math-305"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is invariant.</p><p>This proves the assertion.</p><p>□</p><p><bold>Example 5.4.</bold><italic>Consider a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-306"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } = ( R _ { 2 } ^ { 1 6 } , \bar { g } ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> of signature </italic><inline-formula><tex-math id="math-307"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( - , - , + , + , + , + , + , + , + , + , + , + , + , + , + , + , + , + , + ) \end{document} ]]></tex-math></inline-formula><italic> with respect to the basis </italic><inline-formula><tex-math id="math-308"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ \partial z _ { 1 } ^ { \circ } , \partial z _ { 2 } ^ { \circ } , \partial z _ { 3 } ^ { \circ } , \partial z _ { 4 } ^ { \circ } , \partial z _ { 5 } ^ { \circ } , \partial z _ { 6 } ^ { \circ } , \partial z _ { 7 } ^ { \circ } , \partial z _ { 8 } ^ { \circ } , \partial z _ { 9 } ^ { \circ } , \partial z _ { 1 0 } ^ { \circ } , \partial z _ { 1 1 } ^ { \circ } , \partial z _ { 1 2 } ^ { \circ } , \partial z _ { 1 3 } ^ { \circ } , \partial z _ { 1 4 } ^ { \circ } , \partial z _ { 1 5 } ^ { \circ } , \partial z _ { 1 6 } ^ { \circ } \} \end{document} ]]></tex-math></inline-formula></p><p><inline-formula><tex-math id="math-309"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } ( z _ { 1 } ^ { \circ } , z _ { 2 } ^ { \circ } , z _ { 3 } ^ { \circ } , z _ { 4 } ^ { \circ } , z _ { 5 } ^ { \circ } , z _ { 6 } ^ { \circ } , z _ { 7 } ^ { \circ } , z _ { 8 } ^ { \circ } , z _ { 9 } ^ { \circ } , z _ { 1 0 } ^ { \circ } , z _ { 1 1 } ^ { \circ } , z _ { 1 2 } ^ { \circ } , z _ { 1 3 } ^ { \circ } , z _ { 1 4 } ^ { \circ } , z _ { 1 5 } ^ { \circ } , z _ { 1 6 } ^ { \circ } ) = ( \sigma z _ { 1 } ^ { \circ } , \sigma z _ { 2 } ^ { \circ } , \sigma z _ { 3 } ^ { \circ } , \sigma z _ { 4 } ^ { \circ } , z _ { 5 } ^ { \circ } , z _ { 6 } ^ { \circ } ) = \sigma ^ { \prime } . \end{document} ]]></tex-math></inline-formula><italic></italic><inline-formula><tex-math id="math-310"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( 3 - \sigma ) z _ { 5 } ^ { \circ } , \sigma z _ { 6 } ^ { \circ } , \sigma z _ { 7 } ^ { \circ } , \sigma z _ { 8 } ^ { \circ } , ( 3 - \sigma ) z _ { 9 } ^ { \circ } , \sigma z _ { 1 0 } ^ { \circ } , ( 3 - \sigma ) z _ { 1 1 } ^ { \circ } , \sigma z _ { 1 2 } ^ { \circ } , 3 z _ { 1 3 } ^ { \circ } + z _ { 1 4 } ^ { \circ } , z _ { 1 3 } ^ { \circ } , 3 z _ { 1 5 } ^ { \circ } + z _ { 1 6 } ^ { \circ } , z _ { 1 5 } ^ { \circ } ) \end{document} ]]></tex-math></inline-formula></p><p><italic>Let </italic><inline-formula><tex-math id="math-311"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> be a submanifold </italic><inline-formula><tex-math id="math-312"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \mathbb { R } _ { 2 } ^ { 1 6 } \end{document} ]]></tex-math></inline-formula><italic> defined as</italic></p><disp-formula id="equation-63"><tex-math id="math-313"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle z _ {1} ^ {\circ} = y _ {1} ^ {\prime} - y _ {2} ^ {\prime}, z _ {2} ^ {\circ} = \sigma y _ {4} ^ {\prime}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-64"><tex-math id="math-314"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle z _ {3} ^ {\circ} = y _ {3} ^ {\prime} + y _ {5} ^ {\prime}, z _ {4} ^ {\circ} = y _ {2} ^ {\prime} + y _ {3} ^ {\prime}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-65"><tex-math id="math-315"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle z _ {5} ^ {\circ} = y _ {4} ^ {\prime}, z _ {6} ^ {\circ} = y _ {3} ^ {\prime} - y _ {5} ^ {\prime}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-66"><tex-math id="math-316"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle z _ {7} ^ {\circ} = y _ {2} ^ {\prime} + y _ {1} ^ {\prime}, z _ {8} ^ {\circ} = - y _ {2} ^ {\prime} + y _ {3} ^ {\prime}, z _ {9} ^ {\circ} = - c o s \alpha y _ {6} ^ {\prime}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-67"><tex-math id="math-317"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle z _ {1 0} ^ {\circ} = - c o s \alpha y _ {7} ^ {\prime}, z _ {1 1} ^ {\circ} = s i n \alpha y _ {6} ^ {\prime}, z _ {1 2} ^ {\circ} = s i n \alpha y _ {7} ^ {\prime}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-68"><tex-math id="math-318"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle z _ {1 3} ^ {\circ} = - s i n y _ {7} ^ {\prime} c o s h y _ {8} ^ {\prime}, z _ {1 4} ^ {\circ} = 0, z _ {1 5} ^ {\circ} = c o s y _ {7} ^ {\prime} s i n h y _ {8} ^ {\prime}, z _ {1 6} ^ {\circ} = 0. \end{document} ]]></tex-math></disp-formula><p><italic>Here </italic><inline-formula><tex-math id="math-319"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is spanned by </italic><inline-formula><tex-math id="math-320"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ B _ { 1 } , B _ { 2 } , B _ { 3 } , B _ { 4 } , B _ { 5 } , B _ { 6 } , B _ { 7 } , B _ { 8 } , B _ { 9 } \} \end{document} ]]></tex-math></inline-formula><italic> , where</italic></p><disp-formula id="equation-69"><tex-math id="math-321"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ {1} = - \partial z _ {1} ^ {\circ} + \partial z _ {4} ^ {\circ} + \partial z _ {7} ^ {\circ} - \partial z _ {8} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-70"><tex-math id="math-322"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ {2} = \partial z _ {3} ^ {\circ} + \partial z _ {4} ^ {\circ} + \partial z _ {6} ^ {\circ} + \partial z _ {8} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-71"><tex-math id="math-323"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ {3} = \partial z _ {1} ^ {\circ} + \partial z _ {7} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-72"><tex-math id="math-324"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ {4} = \partial z _ {3} ^ {\circ} - \partial z _ {6} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-73"><tex-math id="math-325"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ {5} = \sigma \partial z _ {2} ^ {\circ} + \partial z _ {5} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-74"><tex-math id="math-326"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ {6} = - c o s \alpha \partial z _ {9} ^ {\circ} + s i n \alpha \partial z _ {1 1} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-75"><tex-math id="math-327"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ {7} = - c o s \alpha \partial z _ {1 0} ^ {\circ} + s i n \alpha \partial z _ {1 2} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-76"><tex-math id="math-328"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ {8} = - c o s y _ {7} ^ {\prime} c o s h y _ {8} ^ {\prime} \partial z _ {1 3} ^ {\circ} + s i n y _ {7} ^ {\prime} s i n h y _ {8} ^ {\prime} \partial z _ {1 5} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-77"><tex-math id="math-329"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ {9} = c o s y _ {7} ^ {\prime} c o s h y _ {8} ^ {\prime} \partial z _ {1 5} ^ {\circ} + s i n y _ {7} ^ {\prime} s i n h y _ {8} ^ {\prime} \partial z _ {1 3} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><p><italic>Therefore, </italic><inline-formula><tex-math id="math-330"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is </italic><inline-formula><tex-math id="math-331"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle a \ 2 - l i g h t l i k e \end{document} ]]></tex-math></inline-formula><italic> submanifold with </italic><inline-formula><tex-math id="math-332"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle R a d ( T M ^ { \circ } ) = S p a n \{ B _ { 1 } , B _ { 2 } \} \end{document} ]]></tex-math></inline-formula><italic> such that </italic><inline-formula><tex-math id="math-333"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } B _ { 1 } = \sigma B _ { 1 } \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-334"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } ( B _ { 2 } ) = \sigma B _ { 2 } \end{document} ]]></tex-math></inline-formula><italic> . This shows that Rad(TM</italic><sup><italic>◦</italic></sup><italic>) is invariant with respect to </italic><inline-formula><tex-math id="math-335"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } } ^ { \prime } \end{document} ]]></tex-math></inline-formula><italic> . Since </italic><inline-formula><tex-math id="math-336"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } B _ { 3 } = \sigma B _ { 3 } , \bar { J } ^ { \prime } B _ { 4 } = \sigma B _ { 4 } , \bar { J } ^ { \prime } B _ { 6 } = ( 3 - \sigma ) B _ { 6 } \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-337"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } B _ { 7 } = \sigma B _ { 7 } \end{document} ]]></tex-math></inline-formula><italic> . Therefore, </italic><inline-formula><tex-math id="math-338"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } = S p a n \{ B _ { 3 } , B _ { 4 } , B _ { 6 } , B _ { 7 } \} \end{document} ]]></tex-math></inline-formula><italic> is invariant with respect to </italic><inline-formula><tex-math id="math-339"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { { \bar { J } } ^ { \prime } } \end{document} ]]></tex-math></inline-formula></p><p><italic>Furthermore, </italic><inline-formula><tex-math id="math-340"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) \end{document} ]]></tex-math></inline-formula><italic> is spanned by </italic><inline-formula><tex-math id="math-341"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ W _ { 1 } , W _ { 2 } , W _ { 3 } , W _ { 4 } , W _ { 5 } \} \end{document} ]]></tex-math></inline-formula><italic> , where</italic></p><disp-formula id="equation-78"><tex-math id="math-342"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W _ {1} = \sin \alpha \partial z _ {9} ^ {\circ} + \cos \alpha \partial z _ {1 1} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-79"><tex-math id="math-343"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W _ {2} = - \partial z _ {2} ^ {\circ} + \sigma \partial z _ {5} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-80"><tex-math id="math-344"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W _ {3} = \sin \alpha \partial z _ {1 0} ^ {\circ} + \cos \alpha \partial z _ {1 2} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-81"><tex-math id="math-345"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W _ {4} = s i n y _ {7} ^ {\prime} s i n h y _ {8} ^ {\prime} \partial z _ {1 4} ^ {\circ} + c o s y _ {7} ^ {\prime} c o s h y _ {8} ^ {\prime} \partial z _ {1 6} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-82"><tex-math id="math-346"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W _ {5} = - c o s y _ {7} ^ {\prime} c o s h y _ {8} ^ {\prime} \partial z _ {1 4} ^ {\circ} + s i n y _ {7} ^ {\prime} s i n h y _ {8} ^ {\prime} \partial z _ {1 6} ^ {\circ}, \end{document} ]]></tex-math></disp-formula><p><italic>We derive, </italic><inline-formula><tex-math id="math-347"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } B _ { 5 } \ = \ 3 B _ { 5 } - W _ { 2 } , \bar { J } ^ { \prime } B _ { 8 } \ = \ 3 B _ { 8 } + W _ { 5 } \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-348"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } B _ { 9 } \ = \ 3 B _ { 9 } \ + \ W _ { 4 } \end{document} ]]></tex-math></inline-formula><italic> , which means </italic><inline-formula><tex-math id="math-349"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B ^ { ' } ~ = ~ S p a n \{ B _ { 5 } , B _ { 8 } , B _ { 9 } \} \end{document} ]]></tex-math></inline-formula><italic> , is not invariant with respect to </italic><inline-formula><tex-math id="math-350"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } ^ { \prime } } \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-351"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } ( B ^ { ' } ) \subset S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-352"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } ( B ^ { ' } ) \subset S ( T M ^ { \circ \bot } ) \end{document} ]]></tex-math></inline-formula></p><p><italic>Therefore, </italic><inline-formula><tex-math id="math-353"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle l t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> is spanned by</italic></p><disp-formula id="equation-83"><tex-math id="math-354"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle N _ {1} = \frac {1}{4} (- \partial z _ {1} ^ {\circ} - \partial z _ {4} ^ {\circ} + \partial z _ {7} ^ {\circ} + \partial z _ {8} ^ {\circ}), N _ {2} = \frac {1}{4} (\partial z _ {3} ^ {\circ} - \partial z _ {4} ^ {\circ} + \partial z _ {6} ^ {\circ} - \partial z _ {8} ^ {\circ}), \end{document} ]]></tex-math></disp-formula><p><italic>which is invariant with respect to </italic><inline-formula><tex-math id="math-355"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } . ~ F u r t h e r , ~ \bar { J } ^ { \prime } W _ { 1 } = ( 3 - \sigma ) W _ { 1 } , ~ \bar { J } ^ { \prime } W _ { 3 } = \sigma W _ { 3 } \end{document} ]]></tex-math></inline-formula><italic> ， which shows that </italic><inline-formula><tex-math id="math-356"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } \mu ^ { \circ } = \mu ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> , where </italic><inline-formula><tex-math id="math-357"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \mu ^ { \circ } = S p a n \{ W _ { 1 } , W _ { 3 } \} \ i . e . , \ \mu ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is invariant with respect to </italic><inline-formula><tex-math id="math-358"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } ^ { \prime } } \end{document} ]]></tex-math></inline-formula><italic> .</italic></p><p><italic>Hence, </italic><inline-formula><tex-math id="math-359"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> become a proper SG-2-lightlike submanifold of </italic><inline-formula><tex-math id="math-360"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle R _ { 2 } ^ { 1 6 } \end{document} ]]></tex-math></inline-formula></p><p><bold>Definition 5.5. </bold><italic>Let </italic><inline-formula><tex-math id="math-361"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> be a SG-lightlike submanifold of a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-362"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M ^ { \circ } } , \bar { J ^ { \prime } } , \bar { g } ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> with an </italic><inline-formula><tex-math id="math-363"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) { - } t y p e \end{document} ]]></tex-math></inline-formula><italic> connection </italic><inline-formula><tex-math id="math-364"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } . \end{document} ]]></tex-math></inline-formula><italic> . Then the distribution B is said to be integrable if and only if </italic><inline-formula><tex-math id="math-365"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle [ X ^ { \circ } , Y ^ { \circ } ] \ \in \ \Gamma ( B ) \end{document} ]]></tex-math></inline-formula><italic> for any </italic><inline-formula><tex-math id="math-366"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( B ) \end{document} ]]></tex-math></inline-formula></p><p><bold>Remark 5.6.</bold><italic>The above definition implies that the distribution B is said to be integrable </italic><inline-formula><tex-math id="math-367"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle i f \end{document} ]]></tex-math></inline-formula><italic> and only if </italic><inline-formula><tex-math id="math-368"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle g ^ { ' } ( [ X ^ { \circ } , Y ^ { \circ } ] , Z ^ { \circ } ) = 0 \end{document} ]]></tex-math></inline-formula><italic> for any </italic><inline-formula><tex-math id="math-369"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( B ) \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-370"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle Z ^ { \circ } \in \end{document} ]]></tex-math></inline-formula><italic></italic><inline-formula><tex-math id="math-371"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Gamma ( B ^ { \perp } ) \end{document} ]]></tex-math></inline-formula></p><p><italic>Theorem 5.7. Let </italic><inline-formula><tex-math id="math-372"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> be a SG-lightlike submanifold of a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-373"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> with an </italic><inline-formula><tex-math id="math-374"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) - t y p e \end{document} ]]></tex-math></inline-formula><italic> connection Ω</italic><sup><italic>¯</italic></sup><italic>. Then, </italic><inline-formula><tex-math id="math-375"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } \end{document} ]]></tex-math></inline-formula><italic> is integrable if and only if the following conditions hold:</italic></p><disp-formula id="equation-84"><tex-math id="math-376"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}(i)\quad & g'\big(\bar{h}^{\circ}(X^\circ, J'Y^\circ), J'N^\circ\big) + 3g'\big(\bar{h}^{\circ}(Y^\circ, J'X^\circ), N^\circ\big) \\&= g'\big(\bar{h}^{\circ}(Y^\circ, J'X^\circ), J'N^\circ\big) + 3g'\big(\bar{h}^{\circ}(X^\circ, J'Y^\circ), N^\circ\big). \\[1.5em](ii)\quad & g'\big(\Omega^{\star}_{X^\circ} J'Y^\circ, f'Z^\circ\big) + g'\big(\bar{h}^{\circ s}(X^\circ, J'Y^\circ), J'Z^\circ\big) + 3g'\big(\Omega^{\star}_{Y^\circ} J'X^\circ, Z^\circ\big) \\&= g'\big(\Omega^{\star}_{Y^\circ} J'X^\circ, f'Z^\circ\big) + g'\big(\bar{h}^{\circ s}(Y^\circ, J'X^\circ), J'Z^\circ\big) + 3g'\big(\Omega^{\star}_{X^\circ} J'Y^\circ, Z^\circ\big),\end{align*} \end{document} ]]></tex-math></disp-formula><p><italic>for any </italic><inline-formula><tex-math id="math-377"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( B _ { o } ) , Z ^ { \circ } \in \Gamma ( B ^ { ' } ) a n d N ^ { \circ } \in \Gamma ( l t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula></p><p><italic>Proof</italic>. The distribution <inline-formula><tex-math id="math-378"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } \end{document} ]]></tex-math></inline-formula> is integrable if and only if</p><disp-formula id="equation-85"><tex-math id="math-379"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {g} ^ {\prime} ([ X ^ {\circ}, Y ^ {\circ} ], N ^ {\circ}) = 0, \quad \bar {g} ^ {\prime} ([ X ^ {\circ}, Y ^ {\circ} ], Z ^ {\circ}) = 0. \end{document} ]]></tex-math></disp-formula><p>Therefore, from equations <xref ref-type="disp-formula" rid="equation-31">(23)</xref>, <xref ref-type="disp-formula" rid="equation-20">(13)</xref>, <xref ref-type="disp-formula" rid="equation-28">(21)</xref>,<xref ref-type="disp-formula" rid="equation-21">(14),</xref><xref ref-type="disp-formula" rid="equation-35">(25)</xref>, <xref ref-type="disp-formula" rid="equation-36">(26)</xref> and <xref ref-type="disp-formula" rid="equation-47">(39)</xref>, we obtain</p><disp-formula id="equation-86"><tex-math id="math-380"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}\bar{g}'\big([X^\circ, Y^\circ], N^\circ\big) &= \bar{g}'\big(\bar{\Omega}_{X^\circ} Y^\circ, N^\circ\big) - l\theta(Y^\circ)\bar{g}'(X^\circ, N^\circ) \\&\quad - m\theta(Y^\circ)\bar{g}'(J'X^\circ, N^\circ) - \bar{g}'\big(\bar{\Omega}_{Y^\circ} X^\circ, N^\circ\big) \\&\quad + l\theta(X^\circ)\bar{g}'(Y^\circ, N^\circ) + m\theta(X^\circ)\bar{g}'(J'Y^\circ, N^\circ) \\&= \bar{g}'\big(\bar{\Omega}_{X^\circ} J'(J'Y^\circ), N^\circ\big) - 3\bar{g}'\big(\bar{\Omega}_{X^\circ} J'Y^\circ, N^\circ\big) \\&\quad - \bar{g}'\big(\bar{\Omega}_{Y^\circ} J'(J'X^\circ), N^\circ\big) + 3\bar{g}'\big(\bar{\Omega}_{Y^\circ} J'X^\circ, N^\circ\big) \\&= g'\big(\bar{h}^{\circ\star}(X^\circ, J'Y^\circ) - \bar{h}^{\circ\star}(Y^\circ, J'X^\circ), J'N^\circ\big) \\&\quad - 3\big\{g'\big(\bar{h}^{\circ\star}(X^\circ, J'Y^\circ) - \bar{h}^{\circ\star}(Y^\circ, J'X^\circ)\big), N^\circ\big\} \\&= 0.\end{align*} \end{document} ]]></tex-math></disp-formula><p>Similarly, on applying <xref ref-type="disp-formula" rid="equation-20">(13)</xref>, <xref ref-type="disp-formula" rid="equation-21">(14)</xref>, <xref ref-type="disp-formula" rid="equation-27">(20)</xref>, <xref ref-type="disp-formula" rid="equation-30">(22)</xref>, <xref ref-type="disp-formula" rid="equation-36">(26)</xref> and <xref ref-type="disp-formula" rid="equation-53">(39)</xref>, we obtain</p><disp-formula id="equation-87"><tex-math id="math-381"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}\bar{g}'\big([X^\circ, Y^\circ], Z^\circ\big) &= \bar{g}'\big(\bar{\Omega}_{X^\circ} Y^\circ - \theta(Y^\circ)\{lX^\circ + mJ'X^\circ\}, Z^\circ\big) \\&\quad - \bar{g}'\big(\bar{\Omega}_{Y^\circ} X^\circ - \theta(X^\circ)\{lY^\circ + mJ'Y^\circ\}, Z^\circ\big) \\&= \bar{g}'\big(\bar{\Omega}_{X^\circ} J'Y^\circ, J'Z^\circ\big) - 3\bar{g}'\big(\bar{\Omega}_{X^\circ} J'Y^\circ, Z^\circ\big) \\&\quad + 3l\theta(J'Y^\circ)\bar{g}'(X^\circ, Z^\circ) - l\theta(J'Y^\circ)\bar{g}'(J'X^\circ, Z^\circ) \\&\quad - m\theta(J'Y^\circ)\bar{g}'(X^\circ, Z^\circ) - \bar{g}'\big(\bar{\Omega}_{Y^\circ} J'X^\circ, J'Z^\circ\big) \\&\quad + 3\bar{g}'\big(\bar{\Omega}_{Y^\circ} J'X^\circ, Z^\circ\big) - 3l\theta(J'X^\circ)\bar{g}'(Y^\circ, Z^\circ) \\&\quad + l\theta(J'X^\circ)\bar{g}'(J'Y^\circ, Z^\circ) + m\theta(J'X^\circ)\bar{g}'(Y^\circ, Z^\circ) \\&= g'\big(\Omega^{\star}_{X^\circ} J'Y^\circ, f'Z^\circ\big) + g'\big(\bar{h}^{\circ s}(X^\circ, J'Y^\circ), J'Z^\circ\big) \\&\quad + 3g'\big(\Omega^{\star}_{Y^\circ} J'X^\circ, Z^\circ\big) - g'\big(\Omega^{\star}_{Y^\circ} J'X^\circ, f'Z^\circ\big) \\&\quad - g'\big(\bar{h}^{\circ s}(Y^\circ, J'X^\circ), J'Z^\circ\big) - 3g'\big(\Omega^{\star}_{X^\circ} J'Y^\circ, Z^\circ\big) \\&= 0.\end{align*} \end{document} ]]></tex-math></disp-formula><p>The required assertion is obtained.</p><p><bold>Theorem 5.8.</bold><italic>The distribution </italic><inline-formula><tex-math id="math-382"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B ^ { ' } \end{document} ]]></tex-math></inline-formula><italic> of a </italic><inline-formula><tex-math id="math-383"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S G \mathrm { - } l i g h t l i k e \end{document} ]]></tex-math></inline-formula><italic> submanifold </italic><inline-formula><tex-math id="math-384"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> in a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-385"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> with an </italic><inline-formula><tex-math id="math-386"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) { - } t y p e \end{document} ]]></tex-math></inline-formula><italic> connection Ω</italic><sup><italic>¯</italic></sup><italic> is integrable if and only if</italic></p><disp-formula id="equation-88"><tex-math id="math-387"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle (i) \Omega_ {Y ^ {\circ}} ^ {*} f ^ {\prime} Z ^ {\circ} + \bar {A} _ {w ^ {\prime} Y ^ {\circ}} Z ^ {\circ} + 3 \Omega_ {Z ^ {\circ}} ^ {*} Y ^ {\circ} - \Omega_ {Z ^ {\circ}} ^ {*} f ^ {\prime} Y ^ {\circ} - \bar {A} _ {w ^ {\prime} Z ^ {\circ}} Y ^ {\circ} - 3 \Omega_ {Y ^ {\circ}} ^ {*} Z ^ {\circ} \end{document} ]]></tex-math></disp-formula><p><italic>has no component in Γ(B ),</italic></p><disp-formula id="equation-89"><tex-math id="math-388"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {A} _ {w ^ {\prime} Y ^ {\circ}} Z ^ {\circ} + \bar {h ^ {\circ}} ^ {*} (Y ^ {\circ}, f ^ {\prime} Z ^ {\circ}) + 3 h ^ {\bar {\circ} *} (Z ^ {\circ}, Y ^ {\circ}) \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-90"><tex-math id="math-389"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {A} _ {w ^ {\prime} Z ^ {\circ}} Y ^ {\circ} + h ^ {\bar {\circ} ^ {*}} (Z ^ {\circ}, f ^ {'} Y ^ {\circ}) + 3 h ^ {\bar {\circ} ^ {*}} (Y ^ {\circ}, Z ^ {\circ}), \end{document} ]]></tex-math></disp-formula><p><italic>for any </italic><inline-formula><tex-math id="math-390"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle Y ^ { \circ } , Z ^ { \circ } \in \Gamma ( B ^ { ' } ) , \ X ^ { \circ } \in \Gamma ( B _ { o } ) , \ N ^ { \circ } \in \Gamma ( l t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula></p><p><italic>Proof</italic>. <inline-formula><tex-math id="math-391"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B ^ { ' } \end{document} ]]></tex-math></inline-formula> is integrable if and only if <inline-formula><tex-math id="math-392"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { g } ^ { \prime } ( [ Y ^ { \circ } , Z ^ { \circ } ] , N ^ { \circ } ) = 0 , \bar { g } ^ { \prime } ( [ Y ^ { \circ } , Z ^ { \circ } ] , X ^ { \circ } ) = 0 . \end{document} ]]></tex-math></inline-formula> Since, Ω is an<sup>¯</sup><inline-formula><tex-math id="math-393"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula> -type connection, therefore applying equations <xref ref-type="disp-formula" rid="equation-21">(14)</xref>, <xref ref-type="disp-formula" rid="equation-22">(15)</xref>, <xref ref-type="disp-formula" rid="equation-35">(25)</xref>, <xref ref-type="disp-formula" rid="equation-36">(26)</xref>, <xref ref-type="disp-formula" rid="equation-43">(32)</xref> and <xref ref-type="disp-formula" rid="equation-30">(22)</xref>, we obtain</p><disp-formula id="equation-91"><tex-math id="math-394"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}\bar{g}'\big([Y^\circ, Z^\circ], N^\circ\big) &= \bar{g}'\big(\bar{\Omega}_{Y^\circ} Z^\circ - l\theta(Z^\circ)Y^\circ - m\theta(Z^\circ)J'Y^\circ, N^\circ\big) \\&\quad - \bar{g}'\big(\bar{\Omega}_{Z^\circ} Y^\circ - l\theta(Y^\circ)Z^\circ - m\theta(Y^\circ)J'Z^\circ, N^\circ\big) \\&= g'\big(\Omega_{Y^\circ} f'Z^\circ, J'N^\circ\big) + g'\big(-\bar{A}_{w'Z^\circ} Y^\circ, J'N^\circ\big) \\&\quad - 3g'\big(\Omega_{Y^\circ} Z^\circ, J'N^\circ\big) - g'\big(\Omega_{Z^\circ} f'Y^\circ, J'N^\circ\big) \\&\quad - g'\big(-\bar{A}_{w'Y^\circ} Z^\circ, J'N^\circ\big) + 3g'\big(\Omega_{Z^\circ} Y^\circ, J'N^\circ\big) \\&= 0.\end{align*} \end{document} ]]></tex-math></disp-formula><p>Now, using equation <xref ref-type="disp-formula" rid="equation-53">(39)</xref>, we get</p><disp-formula id="equation-92"><tex-math id="math-395"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle g ^ {\prime} (\bar {h} ^ {\circ *} (Y ^ {\circ}, f ^ {\prime} Z ^ {\circ}), \bar {J} ^ {\prime} N ^ {\circ}) - g ^ {\prime} (\bar {A} _ {w ^ {\prime} Z ^ {\circ}} Y ^ {\circ}, \bar {J} ^ {\prime} N ^ {\circ}) - 3 g ^ {\prime} (\bar {h} ^ {\circ *} (Y ^ {\circ}, Z ^ {\circ}), \bar {J} ^ {\prime} N ^ {\circ}) \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-93"><tex-math id="math-396"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle - g ^ {\prime} \left(\bar {h} ^ {\circ *} \left(Z ^ {\circ}, f ^ {\prime} Y ^ {\circ}\right), \bar {J} ^ {\prime} N ^ {\circ}\right) + g ^ {\prime} \left(\bar {A} _ {w ^ {\prime} Y ^ {\circ}} Z ^ {\circ}, \bar {J} ^ {\prime} N ^ {\circ}\right) + 3 g ^ {\prime} \left(\bar {h} ^ {\circ *} \left(Z ^ {\circ}, Y ^ {\circ}\right), \bar {J} ^ {\prime} N ^ {\circ}\right) = 0. \end{document} ]]></tex-math></disp-formula><p>Similarly,</p><disp-formula id="equation-94"><tex-math id="math-397"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}\bar{g}'\big([Y^\circ, Z^\circ], X^\circ\big) &= g'\big(\Omega^{\star}_{Y^\circ} f'Z^\circ, J'X^\circ\big) + g'\big(\bar{A}_{w'Y^\circ} Z^\circ, J'X^\circ\big) + 3g'\big(\Omega^{\star}_{Z^\circ} Y^\circ, J'X^\circ\big) \\&\quad + (9m + 3l)\big\{\theta(Z^\circ)g'(f'Y^\circ, X^\circ) - \theta(Y^\circ)g'(f'Z^\circ, X^\circ)\big\} \\&\quad + 3m\big\{\theta(Z^\circ)g'(Y^\circ, X^\circ) - \theta(Y^\circ)g'(Z^\circ, X^\circ)\big\} - g'\big(\Omega^{\star}_{Z^\circ} f'Y^\circ, J'X^\circ\big) \\&\quad - g'\big(\bar{A}_{w'Z^\circ} Y^\circ, J'X^\circ\big) - 3g'\big(\Omega^{\star}_{Y^\circ} Z^\circ, J'X^\circ\big) \\&\quad - (l + 3m)\big\{\theta(J'Z^\circ)g'(f'Y^\circ, X^\circ) - \theta(J'Y^\circ)g'(f'Z^\circ, X^\circ)\big\} \\&\quad - m\big\{\theta(J'Z^\circ)g'(Y^\circ, X^\circ) - \theta(J'Y^\circ)g'(Z^\circ, X^\circ)\big\} \\&= 0.\end{align*} \end{document} ]]></tex-math></disp-formula><p>Then, from the equations <xref ref-type="disp-formula" rid="equation-27">(20)</xref> and <xref ref-type="disp-formula" rid="equation-28">(21)</xref>, we get the desired result.</p><p><bold>Theorem 5.9.</bold><italic>For a SG-lightlike submanifold </italic><inline-formula><tex-math id="math-398"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> ofa locally bronze semi-Riemannian manifold with an </italic><inline-formula><tex-math id="math-399"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) { - } t y p e \end{document} ]]></tex-math></inline-formula><italic> connection </italic><inline-formula><tex-math id="math-400"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } _ { i } \end{document} ]]></tex-math></inline-formula><italic> , the distribution B is integrable if and only if</italic></p><disp-formula id="equation-95"><tex-math id="math-401"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & g ^ {'} (\Omega_ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, f ^ {'} Z ^ {\circ}) + g ^ {'} (h ^ {\circ^ {s}} (X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}), \bar {J} ^ {\prime} Z ^ {\circ}) + 3 g ^ {'} (\Omega_ {Y ^ {\circ}} \bar {J} ^ {\prime} X ^ {\circ}, Z ^ {\circ}) \\ & \qquad = g ^ {'} (\Omega_ {Y ^ {\circ}} \bar {J} ^ {\prime} X ^ {\circ}, f ^ {'} Z ^ {\circ}) + g ^ {'} (h ^ {\circ^ {s}} (Y ^ {\circ}, \bar {J} ^ {\prime} X ^ {\circ}), \bar {J} ^ {\prime} Z ^ {\circ}) \\ & \qquad + 3 g ^ {'} (\Omega_ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, Z ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p><italic>for any </italic><inline-formula><tex-math id="math-402"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( B ) , Z ^ { \circ } \in \Gamma ( B ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-403"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle N ^ { \circ } \in \Gamma ( l t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula><italic> ).</italic></p><p><italic>Proof</italic>. Since <inline-formula><tex-math id="math-404"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> is a locally bronze semi-Riemannian manifold equipped with an (l, m)-type connection <inline-formula><tex-math id="math-405"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } . \end{document} ]]></tex-math></inline-formula> , therefore</p><disp-formula id="equation-96"><tex-math id="math-406"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} \bar {g} ^ {'} ([ X ^ {\circ}, Y ^ {\circ} ], Z ^ {\circ}) = & \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {\prime} (\bar {J} ^ {\prime} Y ^ {\circ}), Z ^ {\circ}) - 3 \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, Z ^ {\circ}) \\ & - \bar {g} ^ {'} (\bar {\Omega} _ {Y ^ {\circ}} \bar {J} ^ {\prime} (\bar {J} ^ {\prime} X ^ {\circ}), Z ^ {\circ}) + 3 \bar {g} ^ {'} (\bar {\Omega} _ {Y ^ {\circ}} \bar {J} ^ {\prime} X ^ {\circ}, Z ^ {\circ}) \\ & - l \theta (Y ^ {\circ}) \bar {g} ^ {'} (X ^ {\circ}, Z ^ {\circ}) - m \theta (Y ^ {\circ}) \bar {g} ^ {'} (\bar {J} ^ {\prime} X ^ {\circ}, Z ^ {\circ}) \\ & + l \theta (X ^ {\circ}) \bar {g} ^ {'} (Y ^ {\circ}, Z ^ {\circ}) + m \theta (X ^ {\circ}) \bar {g} ^ {'} (\bar {J} ^ {\prime} Y ^ {\circ}, Z ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p>Now, using <xref ref-type="disp-formula" rid="equation-30">(22)</xref> and <xref ref-type="disp-formula" rid="equation-36">(26)</xref>, we obtain</p><disp-formula id="equation-97"><tex-math id="math-407"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} \bar {g} ^ {'} ([ X ^ {\circ}, Y ^ {\circ} ], Z ^ {\circ}) & = g ^ {'} (\Omega_ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, f ^ {'} Z ^ {\circ}) + g ^ {'} (\bar {h} ^ {\circ s} (X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}), w ^ {'} Z ^ {\circ}) \\ & \quad + 3 l \theta (\bar {J} ^ {\prime} Y ^ {\circ}) g ^ {'} (X ^ {\circ}, Z ^ {\circ}) - l \theta (\bar {J} ^ {\prime} Y ^ {\circ}) g ^ {'} (\bar {J} ^ {\prime} X ^ {\circ}, Z ^ {\circ}) \\ & \quad - m \theta (\bar {J} ^ {\prime} Y ^ {\circ}) g ^ {'} (X ^ {\circ}, Z ^ {\circ}) - 3 g ^ {'} (\Omega_ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, Z ^ {\circ}) \\ & \quad - g ^ {'} (\Omega_ {Y ^ {\circ}} \bar {J} ^ {\prime} X ^ {\circ}, f ^ {'} Z ^ {\circ}) - g ^ {'} (\bar {h} ^ {\circ s} (Y ^ {\circ}, \bar {J} ^ {\prime} X ^ {\circ}), w ^ {'} Z ^ {\circ}) \\ & \quad - 3 l \theta (\bar {J} ^ {\prime} X ^ {\circ}) g ^ {'} (Y ^ {\circ}, Z ^ {\circ}) + l \theta (\bar {J} ^ {\prime} X ^ {\circ}) g ^ {'} (\bar {J} ^ {\prime} Y ^ {\circ}, Z ^ {\circ}) \\ & \quad + m \theta (\bar {J} ^ {\prime} X ^ {\circ}) g ^ {'} (Y ^ {\circ}, Z ^ {\circ}) + 3 g ^ {'} (\Omega_ {Y ^ {\circ}} \bar {J} ^ {\prime} X ^ {\circ}, Z ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p>Since B is integrable, therefore <inline-formula><tex-math id="math-408"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { g } ^ { \prime } ( [ X ^ { \circ } , Y ^ { \circ } ] , Z ^ { \circ } ) = 0 \end{document} ]]></tex-math></inline-formula> . Also, <inline-formula><tex-math id="math-409"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is SG-lightlike submanifold.</p><p>Thus,</p><disp-formula id="equation-98"><tex-math id="math-410"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & g ^ {'} (\Omega_ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, f ^ {'} Z ^ {\circ}) + g ^ {'} (\bar {h} ^ {\circ^ {s}} (X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}), \bar {J} ^ {\prime} Z ^ {\circ}) + 3 g ^ {'} (\Omega_ {Y ^ {\circ}} \bar {J} ^ {\prime} X ^ {\circ}, Z ^ {\circ}) \\ & \quad - g ^ {'} (\Omega_ {Y ^ {\circ}} \bar {J} ^ {\prime} X ^ {\circ}, f ^ {'} Z ^ {\circ}) - g ^ {'} (\bar {h} ^ {\circ^ {s}} (Y ^ {\circ}, \bar {J} ^ {\prime} X ^ {\circ}), \bar {J} ^ {\prime} Z ^ {\circ}) - 3 g ^ {'} (\Omega_ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, Z ^ {\circ}) = 0. \end{array} \end{document} ]]></tex-math></disp-formula><p>□</p><p><bold>Theorem 5.10.</bold><italic>Let </italic><inline-formula><tex-math id="math-411"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> be a SG-lightlike submanifold of a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-412"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> with an </italic><inline-formula><tex-math id="math-413"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) . \end{document} ]]></tex-math></inline-formula><italic> - type connection Ω</italic><sup><italic>¯</italic></sup><italic>. Then, the distribution </italic><inline-formula><tex-math id="math-414"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } \end{document} ]]></tex-math></inline-formula><italic> is parallel if and only if the following conditions hold:</italic></p><disp-formula id="equation-99"><tex-math id="math-415"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{l l} (i) & g ^ {'} (\bar {h} ^ {\circ^ {*}} (X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}), \bar {J} ^ {\prime} N ^ {\circ}) = 3 g ^ {'} (\bar {h} ^ {\circ^ {*}} (X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}), N ^ {\circ}), \\ (i i) & g ^ {'} (\Omega_ {X ^ {\circ}} ^ {*} \bar {J} ^ {\prime} Y ^ {\circ}, f ^ {'} Z ^ {\circ}) + g ^ {'} (\bar {h} ^ {\circ^ {s}} (X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}), \bar {J} ^ {\prime} Z ^ {\circ}) = 3 g ^ {'} (\Omega_ {X ^ {\circ}} ^ {*} \bar {J} ^ {\prime} Y ^ {\circ}, Z ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p><italic>for all </italic><inline-formula><tex-math id="math-416"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( B _ { o } ) , Z ^ { \circ } \in \Gamma ( B ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> and N</italic><sup><italic>◦</italic></sup><italic> ∈ Γ(ltr(TM</italic><sup><italic>◦</italic></sup><italic>)).</italic></p><p><italic>Proof</italic>. Since the distribution <inline-formula><tex-math id="math-417"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } \end{document} ]]></tex-math></inline-formula> is parallel, therefore for all <inline-formula><tex-math id="math-418"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( B _ { o } ) , Z ^ { \circ } \in \end{document} ]]></tex-math></inline-formula><inline-formula><tex-math id="math-419"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Gamma ( B ^ { ' } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-420"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle N ^ { \circ } \in \Gamma ( l t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula><sup>◦</sup>)),</p><disp-formula id="equation-100"><tex-math id="math-421"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle g ^ {'} (\Omega_ {X ^ {\circ}} Y ^ {\circ}, Z ^ {\circ}) = 0, g ^ {'} (\Omega_ {X ^ {\circ}} Y ^ {\circ}, N ^ {\circ}) = 0,\tag{45} \end{document} ]]></tex-math></disp-formula><p>The concept of locally bronze semi-Riemannian manifold leads to</p><disp-formula id="equation-101"><tex-math id="math-422"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle g ^ {\prime} \left(\Omega_ {X ^ {\circ}} Y ^ {\circ}, N ^ {\circ}\right) = \bar {g} ^ {\prime} \left(\bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {\prime} \left(\bar {J} ^ {\prime} Y ^ {\circ}\right), N ^ {\circ}\right) - 3 \bar {g} ^ {\prime} \left(\bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, N ^ {\circ}\right), \end{document} ]]></tex-math></disp-formula><p>Employing equations <xref ref-type="disp-formula" rid="equation-21">(14)</xref> and <xref ref-type="disp-formula" rid="equation-35">(25)</xref>, we obtain</p><disp-formula id="equation-102"><tex-math id="math-423"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} g ^ {'} (\Omega_ {X ^ {\circ}} Y ^ {\circ}, N ^ {\circ}) & = g ^ {'} (\Omega_ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, \bar {J} ^ {\prime} N ^ {\circ}) + 3 l \theta (\bar {J} ^ {\prime} Y ^ {\circ}) g ^ {'} (X ^ {\circ}, N ^ {\circ}) \\ & \quad + l \theta (Y ^ {\circ}) g ^ {'} (X ^ {\circ}, N ^ {\circ}) - l \theta (\bar {J} ^ {\prime} Y ^ {\circ}) g ^ {'} (\bar {J} ^ {\prime} X ^ {\circ}, N ^ {\circ}) \\ & \quad + m \theta (Y ^ {\circ}) g ^ {'} (\bar {J} ^ {\prime} X ^ {\circ}, N ^ {\circ}) - m \theta (\bar {J} ^ {\prime} Y ^ {\circ}) g ^ {'} (X ^ {\circ}, N ^ {\circ}) \\ & \quad - 3 g ^ {'} (\Omega_ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, N ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p>Equations <xref ref-type="disp-formula" rid="equation-53">(39)</xref> and <xref ref-type="disp-formula" rid="equation-61">(45)</xref> leads to</p><disp-formula id="equation-103"><tex-math id="math-424"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & g ^ {'} (\Omega_ {X ^ {\circ}} Y ^ {\circ}, N ^ {\circ}) = g ^ {'} (\Omega_ {X ^ {\circ}} ^ {*} \bar {J} ^ {\prime} Y ^ {\circ}, \bar {J} ^ {\prime} N ^ {\circ}) + g ^ {'} (\bar {h} ^ {\circ^ {*}} (X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}), \bar {J} ^ {\prime} N ^ {\circ}) \\ & \qquad - 3 g ^ {'} (\Omega_ {X ^ {\circ}} ^ {*} \bar {J} ^ {\prime} Y ^ {\circ}, \bar {J} ^ {\prime} N ^ {\circ}) - 3 g ^ {'} (\bar {h} ^ {\circ^ {*}} (X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}), \bar {J} ^ {\prime} N ^ {\circ}) \\ & \qquad = 0. \end{array} \end{document} ]]></tex-math></disp-formula><p>Similarly, from equations <xref ref-type="disp-formula" rid="equation-20">(13)</xref>, <xref ref-type="disp-formula" rid="equation-21">(14)</xref>, <xref ref-type="disp-formula" rid="equation-30">(22)</xref> and <xref ref-type="disp-formula" rid="equation-35">(25)</xref>, we get</p><disp-formula id="equation-104"><tex-math id="math-425"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} g ^ {'} (\Omega_ {X ^ {\circ}} Y ^ {\circ}, Z ^ {\circ}) & = \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, f ^ {'} Z ^ {\circ}) + \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, w ^ {'} Z ^ {\circ}) \\ & \quad - 3 \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ}, Z ^ {\circ}) + 3 l \theta (\bar {J} ^ {\prime} Y ^ {\circ}) \bar {g} ^ {'} (X ^ {\circ}, Z ^ {\circ}) \\ & \quad + l \theta (Y ^ {\circ}) \bar {g} ^ {'} (X ^ {\circ}, Z ^ {\circ}) - l \theta (\bar {J} ^ {\prime} Y ^ {\circ}) \bar {g} ^ {'} (\bar {J} ^ {\prime} X ^ {\circ}, Z ^ {\circ}) \\ & \quad + m \theta (Y ^ {\circ}) \bar {g} ^ {'} (\bar {J} ^ {\prime} X ^ {\circ}, Z ^ {\circ}) - m \theta (\bar {J} ^ {\prime} Y ^ {\circ}) \bar {g} ^ {'} (X ^ {\circ}, Z ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p>From <xref ref-type="disp-formula" rid="equation-36">(26)</xref>, <xref ref-type="disp-formula" rid="equation-53">(39)</xref> and <xref ref-type="disp-formula" rid="equation-100">(45)</xref>, we attain</p><disp-formula id="equation-105"><tex-math id="math-426"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{l} g ^ {'} (\Omega_ {X ^ {\circ}} Y ^ {\circ}, Z ^ {\circ}) = g ^ {'} (\Omega_ {X ^ {\circ}} ^ {*} \bar {J} ^ {\prime} Y ^ {\circ}, f ^ {'} Z ^ {\circ}) + g ^ {'} (h ^ {\circ^ {s}} (X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}), \bar {J} ^ {\prime} Z ^ {\circ}) - 3 g ^ {'} (\Omega_ {X ^ {\circ}} ^ {*} \bar {J} ^ {\prime} Y ^ {\circ}, Z ^ {\circ}) \\ = 0. \end{array} \end{document} ]]></tex-math></disp-formula><p><bold>Theorem 5.11.</bold><italic>For a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-427"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> with an </italic><inline-formula><tex-math id="math-428"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula><italic> type connection </italic><inline-formula><tex-math id="math-429"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } \end{document} ]]></tex-math></inline-formula><italic> , the distribution </italic><inline-formula><tex-math id="math-430"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B ^ { ' } \end{document} ]]></tex-math></inline-formula><italic> of a SG-lightlike submanifold </italic><inline-formula><tex-math id="math-431"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is parallel if and only if</italic></p><disp-formula id="equation-106"><tex-math id="math-432"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{l} (i) g ^ {'} (\bar {h} ^ {\circ *} (Y ^ {\circ}, f ^ {'} Z ^ {\circ}), \bar {J} ^ {'} N ^ {\circ}) + 3 g ^ {'} (\bar {A} _ {w ^ {'} Z ^ {\circ}} Y ^ {\circ}, N ^ {\circ}) = 3 g ^ {'} (\bar {h} ^ {\circ *} (Y ^ {\circ}, f ^ {'} Z ^ {\circ}), N ^ {\circ}) + \\ g ^ {'} (\bar {A} _ {w ^ {'} Z ^ {\circ}} Y ^ {\circ}, \bar {J} ^ {'} N ^ {\circ}), \\ (i i) g ^ {'} (\Omega_ {Y ^ {\circ}} ^ {*} f ^ {'} Z ^ {\circ}, \bar {J} ^ {'} X ^ {\circ}) + 3 g ^ {'} (\bar {A} _ {w ^ {'} Z ^ {\circ}} Y ^ {\circ}, X ^ {\circ}) = g ^ {'} (\bar {A} _ {w ^ {'} Z ^ {\circ}} Y ^ {\circ}, \bar {J} ^ {'} X ^ {\circ}) \\ + 3 g ^ {'} (\Omega_ {Y ^ {\circ}} ^ {*} f ^ {'} Z ^ {\circ}, X ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p><italic>for any </italic><inline-formula><tex-math id="math-433"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle Y ^ { \circ } , Z ^ { \circ } \in \Gamma ( B ^ { ' } ) , \ X ^ { \circ } \in \Gamma ( B _ { o } ) \ a n d \ N ^ { \circ } \in \Gamma ( l t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula></p><p><italic>Proof</italic>. Let the distribution <inline-formula><tex-math id="math-434"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B ^ { ' } \end{document} ]]></tex-math></inline-formula> is parallel. Therefore, for all <inline-formula><tex-math id="math-435"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \cal Y } ^ { \circ } , { \cal Z } ^ { \circ } \in \Gamma ( B ^ { ' } ) , \ { \cal X } ^ { \circ } \in \end{document} ]]></tex-math></inline-formula><inline-formula><tex-math id="math-436"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Gamma ( B _ { o } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-437"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle N ^ { \circ } \in \Gamma ( l t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula></p><disp-formula id="equation-107"><tex-math id="math-438"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle g ^ {\prime} \left(\Omega_ {Y ^ {\circ}} Z ^ {\circ}, X ^ {\circ}\right) = 0, g ^ {\prime} \left(\Omega_ {Y ^ {\circ}} Z ^ {\circ}, N ^ {\circ}\right) = 0, \end{document} ]]></tex-math></disp-formula><p>Now, using equations <xref ref-type="disp-formula" rid="equation-20">(13)</xref> and <xref ref-type="disp-formula" rid="equation-35">(25)</xref>, we obtain</p><disp-formula id="equation-108"><tex-math id="math-439"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{c} g ^ {'} (\Omega_ {Y ^ {\circ}} Z ^ {\circ}, N ^ {\circ}) = \bar {g} ^ {'} (\bar {J} ^ {'} (\bar {\Omega} _ {Y ^ {\circ}} \bar {J} ^ {'} Z ^ {\circ}), N ^ {\circ}) + \bar {g} ^ {'} (l \{3 \theta (\bar {J} ^ {'} Z ^ {\circ}) Y ^ {\circ} + \theta (Z ^ {\circ}) Y ^ {\circ} \\ - \theta (\bar {J} ^ {'} Z ^ {\circ}) \bar {J} ^ {'} Y ^ {\circ} \}, N ^ {\circ}) + \bar {g} ^ {'} (m \{\theta (Z ^ {\circ}) \bar {J} ^ {'} Y ^ {\circ} \\ - \theta (\bar {J} ^ {'} Z ^ {\circ}) Y ^ {\circ} \}, N ^ {\circ}) - 3 \bar {g} ^ {'} (\bar {\Omega} _ {Y ^ {\circ}} \bar {J} ^ {'} Z ^ {\circ}, N ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p>Employing <xref ref-type="disp-formula" rid="equation-21">(14)</xref>, <xref ref-type="disp-formula" rid="equation-30">(22)</xref>, <xref ref-type="disp-formula" rid="equation-36">(26)</xref> and <xref ref-type="disp-formula" rid="equation-44">(33)</xref>, we attain</p><disp-formula id="equation-109"><tex-math id="math-440"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} g ^ {'} (\Omega_ {Y ^ {\circ}} Z ^ {\circ}, N ^ {\circ}) & = g ^ {'} (\Omega_ {Y ^ {\circ}} f ^ {'} Z ^ {\circ}, \bar {J} ^ {'} N ^ {\circ}) + g ^ {'} (\bar {h} ^ {\circ^ {l}} (Y ^ {\circ}, f ^ {'} Z ^ {\circ}), \bar {J} ^ {'} N ^ {\circ}) \\ & \quad + g ^ {'} (\bar {h} ^ {\circ^ {s}} (Y ^ {\circ}, f ^ {'} Z ^ {\circ}), \bar {J} ^ {'} N ^ {\circ}) + g ^ {'} (- \bar {A} _ {w ^ {'} Z ^ {\circ}} Y ^ {\circ}, \bar {J} ^ {'} N ^ {\circ}) \\ & \quad + g ^ {'} (\bar {\Omega} _ {Y ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ}, \bar {J} ^ {'} N ^ {\circ}) + g ^ {'} (\bar {D} ^ {\circ^ {l}} (Y ^ {\circ}, w ^ {'} Z ^ {\circ}), \bar {J} ^ {'} N ^ {\circ}) \\ & \quad - 3 g ^ {'} (\Omega_ {Y ^ {\circ}} f ^ {'} Z ^ {\circ}, N ^ {\circ}) - 3 g ^ {'} (\bar {h} ^ {\circ^ {l}} (Y ^ {\circ}, f ^ {'} Z ^ {\circ}), N ^ {\circ}) \\ & \quad - 3 g ^ {'} (\bar {h} ^ {\circ^ {s}} (Y ^ {\circ}, f ^ {'} Z ^ {\circ}), N ^ {\circ}) - 3 g ^ {'} (- \bar {A} _ {w ^ {'} Z ^ {\circ}} Y ^ {\circ}, N ^ {\circ}) \\ & \quad - 3 g ^ {'} (\bar {\Omega} _ {Y ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ}, N ^ {\circ}) - 3 g ^ {'} (\bar {D} ^ {\circ^ {l}} (Y ^ {\circ}, w ^ {'} Z ^ {\circ}), N ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p>Further, from equation <xref ref-type="disp-formula" rid="equation-53">(39)</xref>, we get</p><disp-formula id="equation-110"><tex-math id="math-441"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & g ^ {'} (\Omega_ {Y ^ {\circ}} Z ^ {\circ}, N ^ {\circ}) = g ^ {'} (\Omega_ {Y ^ {\circ}} ^ {*} f ^ {'} Z ^ {\circ}, \bar {J} ^ {'} N ^ {\circ}) + g ^ {'} (\bar {h} ^ {\circ *} (Y ^ {\circ}, f ^ {'} Z ^ {\circ}), \bar {J} ^ {'} N ^ {\circ}) \\ & \qquad + g ^ {'} (- \bar {A} _ {w ^ {'} Z ^ {\circ}} Y ^ {\circ}, \bar {J} ^ {'} N ^ {\circ}) - 3 g ^ {'} (\Omega_ {Y ^ {\circ}} ^ {*} f ^ {'} Z ^ {\circ}, N ^ {\circ}) \\ & \qquad - 3 g ^ {'} (\bar {h} ^ {\circ *} (Y ^ {\circ}, f ^ {'} Z ^ {\circ}), N ^ {\circ}) - 3 g ^ {'} (- \bar {A} _ {w ^ {'} Z ^ {\circ}} Y ^ {\circ}, N ^ {\circ}) \\ & \qquad = 0. \end{array} \end{document} ]]></tex-math></disp-formula><p>Similarly,</p><disp-formula id="equation-111"><tex-math id="math-442"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} g ^ {'} (\Omega_ {Y ^ {\circ}} Z ^ {\circ}, X ^ {\circ}) & = g ^ {'} (\Omega_ {Y ^ {\circ}} \bar {J} ^ {'} Z ^ {\circ}, \bar {J} ^ {'} X ^ {\circ}) + 3 l \theta (\bar {J} ^ {'} Z ^ {\circ}) g ^ {'} (Y ^ {\circ}, X ^ {\circ}) \\ & \quad + l \theta (Z ^ {\circ}) g ^ {'} (Y ^ {\circ}, X ^ {\circ}) - l \theta (\bar {J} ^ {'} Z ^ {\circ}) g ^ {'} (\bar {J} ^ {'} Y ^ {\circ}, X ^ {\circ}) \\ & \quad + m \theta (Z ^ {\circ}) g ^ {'} (\bar {J} ^ {'} Y ^ {\circ}, X ^ {\circ}) - m \theta (\bar {J} ^ {'} Z ^ {\circ}) g ^ {'} (Y ^ {\circ}, X ^ {\circ}) \\ & \quad - 3 g ^ {'} (\Omega_ {Y ^ {\circ}} \bar {J} ^ {'} Z ^ {\circ}, X ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p>Equations <xref ref-type="disp-formula" rid="equation-36">(26),</xref><xref ref-type="disp-formula" rid="equation-44">(33)</xref> and <xref ref-type="disp-formula" rid="equation-53">(39)</xref> leads to</p><disp-formula id="equation-112"><tex-math id="math-443"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & g ^ {'} (\Omega_ {Y ^ {\circ}} Z ^ {\circ}, X ^ {\circ}) = g ^ {'} (\Omega_ {Y ^ {\circ}} ^ {*} f ^ {'} Z ^ {\circ} + \bar {h} ^ {\circ^ {*}} (Y ^ {\circ}, f ^ {'} Z ^ {\circ}), \bar {J} ^ {'} X ^ {\circ}) + g ^ {'} (- \bar {A} _ {w ^ {'} Z ^ {\circ}} Y ^ {\circ}, \bar {J} ^ {'} X ^ {\circ}) \\ & \qquad - 3 g ^ {'} (\Omega_ {Y ^ {\circ}} ^ {*} f ^ {'} Z ^ {\circ} + \bar {h} ^ {\circ^ {*}} (Y ^ {\circ}, f ^ {'} Z ^ {\circ}), X ^ {\circ}) - 3 g ^ {'} (- \bar {A} _ {w ^ {'} Z ^ {\circ}} Y ^ {\circ}, X ^ {\circ}) \\ & \qquad = 0. \end{array} \end{document} ]]></tex-math></disp-formula><p><bold>Definition 5.12.</bold><xref ref-type="bibr" rid="BIBR-11">[11]</xref><italic></italic><inline-formula><tex-math id="math-444"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is a screen B-geodesic SG-lightlike submanifold if its second fundamental form satisfies</italic></p><disp-formula id="equation-113"><tex-math id="math-445"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ {\circ} (X ^ {\circ}, Y ^ {\circ}) = 0, \quad \forall X ^ {\circ}, Y ^ {\circ} \in \Gamma (B),\tag{46} \end{document} ]]></tex-math></disp-formula><p><bold>Remark 5.13.</bold><italic>M</italic><sup><italic>◦</italic></sup><italic> is B-geodesic SG-lightlike submanifold of </italic><inline-formula><tex-math id="math-446"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> endowed with an </italic><inline-formula><tex-math id="math-447"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula><italic> -type connection if</italic></p><disp-formula id="equation-114"><tex-math id="math-448"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {h ^ {\circ}} ^ {l} (X ^ {\circ}, Y ^ {\circ}) = \bar {h ^ {\circ}} ^ {s} (X ^ {\circ}, Y ^ {\circ}) = 0, \forall X ^ {\circ}, Y ^ {\circ} \in \Gamma (B).\tag{47} \end{document} ]]></tex-math></disp-formula><p><bold>Theorem 5.14.</bold><italic>The distribution B ofa SG-lightlike submanifold ofa locally bronze semi-Riemannian manifold with an </italic><inline-formula><tex-math id="math-449"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula><italic> -type connection Ω</italic><sup><italic>¯</italic></sup><italic> defines a totally geodesic foliation in </italic><inline-formula><tex-math id="math-450"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> if and only if </italic><inline-formula><tex-math id="math-451"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is B-geodesic and B is parallel with respect to </italic><inline-formula><tex-math id="math-452"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } \end{document} ]]></tex-math></inline-formula><italic> on </italic><inline-formula><tex-math id="math-453"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ }. \end{document} ]]></tex-math></inline-formula></p><p><italic>Proof</italic>. If B defines totally geodesic foliation in <inline-formula><tex-math id="math-454"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> , then for all <inline-formula><tex-math id="math-455"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( B ) \end{document} ]]></tex-math></inline-formula><inline-formula><tex-math id="math-456"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } _ { X ^ { \circ } } Y ^ { \circ } \in \Gamma ( B ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-457"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { g } ^ { \prime } ( \bar { \Omega } _ { X ^ { \circ } } Y ^ { \circ } , \xi ^ { \circ } ) = 0 , \bar { g } ^ { \prime } ( \bar { \Omega } _ { X ^ { \circ } } Y ^ { \circ } , W ^ { \circ } ) = 0 , \bar { g } ^ { \prime } ( \bar { \Omega } _ { X ^ { \circ } } Y ^ { \circ } , Z ^ { \circ } ) = \end{document} ]]></tex-math></inline-formula> 0, for all <inline-formula><tex-math id="math-458"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \xi ^ { \circ } \in \Gamma ( R a d ( T M ^ { \circ } ) ) , Z ^ { \circ } \in \Gamma ( B ^ { ' } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-459"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula> . T (9c) (99) d (20)</p><p>Using equations <xref ref-type="disp-formula" rid="equation-36">(26)</xref>, <xref ref-type="disp-formula" rid="equation-38">(28)</xref> and <xref ref-type="disp-formula" rid="equation-38">(29)</xref>, we get</p><disp-formula id="equation-115"><tex-math id="math-460"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}\bar{g}'\big(\bar{\Omega}_{X^\circ} Y^\circ, \xi^\circ\big) &= g'\big(\bar{h}^{\circ l}(X^\circ, Y^\circ), \xi^\circ\big) \\&= g'\big(h^{\circ l}(X^\circ, Y^\circ), \xi^\circ\big) + m\theta(Y^\circ)g'\big(w'_l X^\circ, \xi^\circ\big), \\[1em]\bar{g}'\big(\bar{\Omega}_{X^\circ} Y^\circ, W^\circ\big) &= g'\big(\bar{h}^{\circ s}(X^\circ, Y^\circ), W^\circ\big) \\&= g'\big(h^{\circ s}(X^\circ, Y^\circ), W^\circ\big) + m\theta(Y^\circ)g'\big(w'_s X^\circ, W^\circ\big),\end{align*} \end{document} ]]></tex-math></disp-formula><p>Since <inline-formula><tex-math id="math-461"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is SG-lightlike submanifold of <inline-formula><tex-math id="math-462"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> . Therefore, the distribution B is invariant with respect to bronze structure <inline-formula><tex-math id="math-463"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } ^ { \prime } } \end{document} ]]></tex-math></inline-formula> . Hence, <inline-formula><tex-math id="math-464"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle w _ { l } ^ { ' } X ^ { \circ } \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-465"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle w _ { s } ^ { ' } X ^ { \circ } \end{document} ]]></tex-math></inline-formula> vanishes.</p><p>Thus, <inline-formula><tex-math id="math-466"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { h ^ { \circ } } ^ { s } ( X ^ { \circ } , Y ^ { \circ } ) = \bar { h ^ { \circ } } ^ { l } ( X ^ { \circ } , Y ^ { \circ } ) = 0 \end{document} ]]></tex-math></inline-formula> , which implies that <inline-formula><tex-math id="math-467"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is B-geodesic and B is parallel with respect to Ω on <inline-formula><tex-math id="math-468"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula></p><p>Conversely, let <inline-formula><tex-math id="math-469"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> be B-geodesic and parallel with respect to Ω on <inline-formula><tex-math id="math-470"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> . Therefore, <inline-formula><tex-math id="math-471"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { h ^ { \circ } } ^ { s } ( X ^ { \circ } , Y ^ { \circ } ) = \bar { h ^ { \circ } } ^ { l } ( X ^ { \circ } , Y ^ { \circ } ) = 0 ~ \forall ~ X ^ { \circ } , Y ^ { \circ } \in \Gamma ( B ) \end{document} ]]></tex-math></inline-formula> , which implies that <inline-formula><tex-math id="math-472"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \Omega } _ { X ^ { \circ } } Y ^ { \circ } \in \end{document} ]]></tex-math></inline-formula><inline-formula><tex-math id="math-473"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \Gamma ( B ) \end{document} ]]></tex-math></inline-formula></p><p><bold>Definition 5.15.</bold><xref ref-type="bibr" rid="BIBR-1">[11]</xref><italic> " </italic><inline-formula><tex-math id="math-474"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic>is a mixed geodesic SG-lightlike submanifold of a locally bronze semi-Riemannian manifold if its second fundamental form satisfies</italic></p><disp-formula id="equation-116"><tex-math id="math-475"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ {\circ} (X ^ {\circ}, Y ^ {\circ}) = 0, \forall X ^ {\circ} \in \Gamma (B), Y ^ {\circ} \in \Gamma (B ^ {^ {\prime}}) ”\tag{48} \end{document} ]]></tex-math></disp-formula><p><bold>Remark 5.16.</bold><italic>If its second fundamental forms satisfies the conditions</italic></p><disp-formula id="equation-117"><tex-math id="math-476"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {h ^ {\circ}} ^ {l} (X ^ {\circ}, Y ^ {\circ}) = \bar {h ^ {\circ}} ^ {s} (X ^ {\circ}, Y ^ {\circ}) = 0, \forall X ^ {\circ} \in \Gamma (B), Y ^ {\circ} \in \Gamma (B ^ {'}),\tag{49} \end{document} ]]></tex-math></disp-formula><p><italic>then </italic><inline-formula><tex-math id="math-477"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is said to be mixed geodesic </italic><inline-formula><tex-math id="math-478"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S G \mathrm { - } l i g h t l i k e \end{document} ]]></tex-math></inline-formula><italic> submanifold with an </italic><inline-formula><tex-math id="math-479"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) { - } t y p e \end{document} ]]></tex-math></inline-formula><italic> connection.</italic></p><p><bold>Theorem 5.17. </bold><italic>Let </italic><inline-formula><tex-math id="math-480"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> be a SG-lightlike submanifold of a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-481"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M } ^ { \circ } , \bar { g } ^ { ' } , \bar { J } ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> equipped with an </italic><inline-formula><tex-math id="math-482"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula><italic> -type connection Ω</italic><sup><italic>¯</italic></sup><italic>. Then </italic><inline-formula><tex-math id="math-483"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is mixed geodesic if and only if</italic></p><disp-formula id="equation-118"><tex-math id="math-484"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} (i) & g ^ {'} (\bar {h} ^ {\circ l} (X ^ {\circ}, f ^ {'} Z ^ {\circ}), \xi^ {\circ}) + l \theta (Z ^ {\circ}) g ^ {'} (\bar {J} ^ {'} X ^ {\circ}, \xi^ {\circ}) + 3 m \theta (Z ^ {\circ}) g ^ {'} (\bar {J} ^ {'} X ^ {\circ}, \xi^ {\circ}) + \\ & m \theta (Z ^ {\circ}) g ^ {'} (X ^ {\circ}, \xi^ {\circ}) = - g ^ {'} (\bar {D} ^ {\circ l} (X ^ {\circ}, w ^ {'} Z ^ {\circ}), \xi^ {\circ}) + l \theta (\bar {J} ^ {'} Z ^ {\circ}) g ^ {'} (X ^ {\circ}, \xi^ {\circ}) \\ & \quad + m \theta (\bar {J} ^ {'} Z ^ {\circ}) g ^ {'} (\bar {J} ^ {'} X ^ {\circ}, \xi^ {\circ}), \\ (i i) & 3 g ^ {'} (\bar {h} ^ {\circ s} (X ^ {\circ}, f ^ {'} Z ^ {\circ}) + \bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ}, W ^ {\circ}) + g ^ {'} (\bar {A} _ {w ^ {'} Z ^ {\circ}} X ^ {\circ}, f ^ {'} W ^ {\circ}) = \\ & g ^ {'} (\Omega_ {X ^ {\circ}} f ^ {'} Z ^ {\circ} + \bar {h} ^ {\circ s} (X ^ {\circ}, f ^ {'} Z ^ {\circ}), \bar {J} ^ {'} W ^ {\circ}) + g ^ {'} (\bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ}, w ^ {'} W ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p><italic>for all </italic><inline-formula><tex-math id="math-485"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \in \Gamma ( B ) , ~ Z ^ { \circ } \in \Gamma ( B ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-486"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula></p><p><italic>Proof</italic>. Since <inline-formula><tex-math id="math-487"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is mixed geodesic, therefore</p><p><inline-formula><tex-math id="math-488"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle g ^ { ' } ( \bar { h ^ { \circ } } ^ { \iota } ( X ^ { \circ } , Z ^ { \circ } ) , \xi ^ { \circ } ) = 0 , g ^ { ' } ( \bar { h ^ { \circ } } ^ { s } ( X ^ { \circ } , Z ^ { \circ } ) , W ^ { \circ } ) = 0 \end{document} ]]></tex-math></inline-formula> , for all <inline-formula><tex-math id="math-489"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \in \Gamma ( B ) , ~ Z ^ { \circ } \in \Gamma ( B ^ { ' } ) \end{document} ]]></tex-math></inline-formula><inline-formula><tex-math id="math-490"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \xi ^ { \circ } \in \Gamma ( R a d ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-491"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula></p><p>Using Gauss formula, we derive</p><disp-formula id="equation-119"><tex-math id="math-492"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {g} ^ {\prime} (\bar {\Omega} _ {X ^ {\circ}} Z ^ {\circ}, \xi^ {\circ}) = 0, \bar {g} ^ {\prime} (\bar {\Omega} _ {X ^ {\circ}} Z ^ {\circ}, W ^ {\circ}) = 0 \end{document} ]]></tex-math></disp-formula><p>From equations <xref ref-type="disp-formula" rid="equation-26">(19)</xref>, <xref ref-type="disp-formula" rid="equation-30">(22)</xref> and <xref ref-type="disp-formula" rid="equation-35">(25)</xref>, we infer</p><disp-formula id="equation-120"><tex-math id="math-493"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {\bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} Z ^ {\circ}, \xi^ {\circ}) = \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} Z ^ {\circ}, \bar {J} ^ {\prime} \xi^ {\circ})} \\ & {\qquad = \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} f ^ {'} Z ^ {\circ}, \xi^ {\circ}) + \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} w ^ {'} Z ^ {\circ}, \xi^ {\circ}) + l \theta (Z ^ {\circ}) \bar {g} ^ {'} (\bar {J} ^ {\prime} X ^ {\circ}, \xi^ {\circ})} \\ & {\qquad + 3 m \theta (Z ^ {\circ}) \bar {g} ^ {'} (\bar {J} ^ {'} X ^ {\circ}, \xi^ {\circ}) + m \theta (Z ^ {\circ}) \bar {g} ^ {'} (X ^ {\circ}, \xi^ {\circ}) - l \theta (\bar {J} ^ {'} Z ^ {\circ}) \bar {g} ^ {'} (X ^ {\circ}, \xi^ {\circ})} \\ & {\qquad - m \theta (\bar {J} ^ {'} Z ^ {\circ}) \bar {g} ^ {'} (\bar {J} ^ {'} X ^ {\circ}, \xi^ {\circ})} \\ & {\qquad = 0,} \end{array} \end{document} ]]></tex-math></disp-formula><p>Similarly, using equations <xref ref-type="disp-formula" rid="equation-20">(13)</xref>, <xref ref-type="disp-formula" rid="equation-21">(14)</xref>, <xref ref-type="disp-formula" rid="equation-30">(22)</xref> and <xref ref-type="disp-formula" rid="equation-35">(25)</xref>, we get</p><disp-formula id="equation-121"><tex-math id="math-494"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {\bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} Z ^ {\circ}, W ^ {\circ}) = \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {'} (\bar {J} ^ {'} Z ^ {\circ}), W ^ {\circ}) - 3 \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {'} Z ^ {\circ}, W ^ {\circ})} \\ & {\qquad = \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} f ^ {'} Z ^ {\circ}, f ^ {'} W ^ {\circ}) + \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} f ^ {'} Z ^ {\circ}, w ^ {'} W ^ {\circ}) + \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} w ^ {'} Z ^ {\circ}, f ^ {'} W ^ {\circ})} \\ & {\qquad + \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} w ^ {'} Z ^ {\circ}, w ^ {'} W ^ {\circ}) - 3 \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} f ^ {'} Z ^ {\circ}, W ^ {\circ}) - 3 \bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} w ^ {'} Z ^ {\circ}, W ^ {\circ}),} \end{array} \end{document} ]]></tex-math></disp-formula><p>Employing equations <xref ref-type="disp-formula" rid="equation-36">(26)</xref> and <xref ref-type="disp-formula" rid="equation-44">(33)</xref>, we attain</p><disp-formula id="equation-122"><tex-math id="math-495"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {\bar {g} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} Z ^ {\circ}, W ^ {\circ}) = g ^ {'} (\Omega_ {X ^ {\circ}} f ^ {'} Z ^ {\circ}, f ^ {'} W ^ {\circ}) + g ^ {'} (\bar {h} ^ {\circ s} (X ^ {\circ}, f ^ {'} Z ^ {\circ}), w ^ {'} W ^ {\circ})} \\ & {\qquad + g ^ {'} (- \bar {A} _ {w ^ {'} Z ^ {\circ}} X ^ {\circ}, f ^ {'} W ^ {\circ}) + g ^ {'} (\bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ}, w ^ {'} W ^ {\circ})} \\ & {\qquad - 3 g ^ {'} (\bar {h} ^ {\circ s} (X ^ {\circ}, f ^ {'} Z ^ {\circ}), W ^ {\circ}) - 3 g ^ {'} (\bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ}, W ^ {\circ})} \\ & {\qquad = 0.} \end{array} \end{document} ]]></tex-math></disp-formula><p><bold>Theorem 5.18.</bold><italic>Let </italic><inline-formula><tex-math id="math-496"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> be a SG-lightlike submanifold of a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-497"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> equipped with an </italic><inline-formula><tex-math id="math-498"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula><italic> -type connection Ω</italic><sup><italic>¯</italic></sup><italic>. Then, for any </italic><inline-formula><tex-math id="math-499"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \in \Gamma ( B _ { o } ) , Z ^ { \circ } \in \Gamma ( B ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> ， </italic><inline-formula><tex-math id="math-500"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle f ^ { ' } ( \Omega _ { X ^ { 0 } } f ^ { ' } Z ^ { 0 } - \bar { A } _ { w ^ { \prime } Z ^ { 0 } } X ^ { 0 } ) + B ^ { ' } ( \bar { h ^ { \circ } } ^ { s } ( X ^ { 0 } , f ^ { ' } Z ^ { 0 } ) + \bar { \Omega } _ { X ^ { 0 } } ^ { s } w ^ { ' } Z ^ { 0 } ) + 3 \bar { A } _ { w ^ { \prime } Z ^ { 0 } } X ^ { 0 } + 3 l \theta ( \bar { J ^ { \prime } } Z ^ { 0 } ) X ^ { 0 } + \bar { O } ( \bar { h ^ { \prime } } Z ^ { 0 } ) , \end{document} ]]></tex-math></inline-formula><italic></italic><inline-formula><tex-math id="math-501"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle l \theta ( Z ^ { \circ } ) X ^ { \circ } + m \theta ( Z ^ { \circ } ) \bar { J } ^ { \prime } X ^ { \circ } = 3 \Omega _ { X ^ { \circ } } f ^ { ' } Z ^ { \circ } + l \theta ( \bar { J } ^ { \prime } Z ^ { \circ } ) \bar { J } ^ { \prime } X ^ { \circ } + m \theta ( \bar { J } ^ { \prime } Z ^ { \circ } ) X ^ { \circ } + \Omega _ { X ^ { \circ } } Z ^ { \circ } . \end{document} ]]></tex-math></inline-formula></p><p><italic>Proof.</italic> Using <xref ref-type="disp-formula" rid="equation-20">(13)</xref>, <xref ref-type="disp-formula" rid="equation-30">(22)</xref> and <xref ref-type="disp-formula" rid="equation-35">(25)</xref>, we get</p><disp-formula id="equation-123"><tex-math id="math-502"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {\bar {\Omega} _ {X ^ {\circ}} Z ^ {\circ} = \bar {J} ^ {\prime} (\bar {\Omega} _ {X ^ {\circ}} f ^ {'} Z ^ {\circ}) + \bar {J} ^ {\prime} (\bar {\Omega} _ {X ^ {\circ}} w ^ {'} Z ^ {\circ}) + 3 l \theta (\bar {J} ^ {'} Z ^ {\circ}) X ^ {\circ} + l \theta (Z ^ {\circ}) X ^ {\circ} - l \theta (\bar {J} ^ {'} Z ^ {\circ}) \bar {J} ^ {'} X ^ {\circ}} \\ & {\qquad + m \theta (Z ^ {\circ}) \bar {J} ^ {'} X ^ {\circ} - m \theta (\bar {J} ^ {'} Z ^ {\circ}) X ^ {\circ} - 3 \bar {\Omega} _ {X ^ {\circ}} f ^ {'} Z ^ {\circ} - 3 \bar {\Omega} _ {X ^ {\circ}} w ^ {'} Z ^ {\circ},} \end{array} \end{document} ]]></tex-math></disp-formula><p>From <xref ref-type="disp-formula" rid="equation-24">(17)</xref>, <xref ref-type="disp-formula" rid="equation-25">(18)</xref>, <xref ref-type="disp-formula" rid="equation-36">(26)</xref> and <xref ref-type="disp-formula" rid="equation-44">(33)</xref>, we obtain</p><disp-formula id="equation-124"><tex-math id="math-503"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {\bar {\Omega} _ {X ^ {\circ}} Z ^ {\circ} = f ^ {'} (\Omega_ {X ^ {\circ}} f ^ {'} Z ^ {\circ}) + w ^ {'} (\Omega_ {X ^ {\circ}} f ^ {'} Z ^ {\circ}) + B ^ {'} (h ^ {\circ l} (X ^ {\circ}, f ^ {'} Z ^ {\circ})) + C ^ {'} (h ^ {\circ l} (X ^ {\circ}, f ^ {'} Z ^ {\circ}))} \\ & {\qquad + B ^ {'} (h ^ {\circ s} (X ^ {\circ}, f ^ {'} Z ^ {\circ})) + C ^ {'} (h ^ {\circ s} (X ^ {\circ}, f ^ {'} Z ^ {\circ})) + f ^ {'} (- \bar {A} _ {w ^ {'} Z ^ {\circ}} X ^ {\circ})} \\ & {\qquad + w ^ {'} (- \bar {A} _ {w ^ {'} Z ^ {\circ}} X ^ {\circ}) + B ^ {'} (\bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ}) + C ^ {'} (\bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ}) + B ^ {'} (\bar {D} ^ {\circ l} (X ^ {\circ}, w ^ {'} Z ^ {\circ}))} \\ & {\qquad + C ^ {'} (\bar {D} ^ {\circ l} (X ^ {\circ}, w ^ {'} Z ^ {\circ})) + 3 l \theta (\bar {J} ^ {'} Z ^ {\circ}) X ^ {\circ} + l \theta (Z ^ {\circ}) X ^ {\circ} - l \theta (\bar {J} ^ {'} Z ^ {\circ}) \bar {J} ^ {'} X ^ {\circ}} \\ & {\qquad + m \theta (Z ^ {\circ}) \bar {J} ^ {'} X ^ {\circ} - m \theta (\bar {J} ^ {'} Z ^ {\circ}) X ^ {\circ} - 3 \Omega_ {X ^ {\circ}} f ^ {'} Z ^ {\circ} - 3 \bar {h} ^ {\circ l} (X ^ {\circ}, f ^ {'} Z ^ {\circ})} \\ & {\qquad - 3 \bar {h} ^ {\circ s} (X ^ {\circ}, f ^ {'} Z ^ {\circ}) + 3 \bar {A} _ {w ^ {'} Z ^ {\circ}} X ^ {\circ} - 3 \bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ} - 3 \bar {D} ^ {\circ l} (X ^ {\circ}, w ^ {'} Z ^ {\circ}),} \end{array} \end{document} ]]></tex-math></disp-formula><p>Comparing tangential parts in the above equation,</p><disp-formula id="equation-125"><tex-math id="math-504"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {\Omega_ {X ^ {\circ}} Z ^ {\circ} = f ^ {'} (\Omega_ {X ^ {\circ}} f ^ {'} Z ^ {\circ} - \bar {A} _ {w ^ {'} Z ^ {\circ}} X ^ {\circ}) + B ^ {'} (h ^ {\circ s} (X ^ {\circ}, f ^ {'} Z ^ {\circ}) + \bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ}) + 3 \bar {A} _ {w ^ {'} Z ^ {\circ}} X ^ {\circ}} \\ & {\qquad + 3 l \theta (\bar {J} ^ {'} Z ^ {\circ}) X ^ {\circ} + l \theta (Z ^ {\circ}) X ^ {\circ} + m \theta (Z ^ {\circ}) \bar {J} ^ {'} X ^ {\circ} - 3 \Omega_ {X ^ {\circ}} f ^ {'} Z ^ {\circ} - l \theta (\bar {J} ^ {'} Z ^ {\circ}) \bar {J} ^ {'} X ^ {\circ}} \\ & {\qquad - m \theta (\bar {J} ^ {'} Z ^ {\circ}) X ^ {\circ}.} \end{array} \end{document} ]]></tex-math></disp-formula><p><bold>Theorem 5.19.</bold><italic>For a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-505"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M } ^ { \circ } , \bar { g } ^ { ' } , \bar { J } ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> with an (l, m)-type connection Ω</italic><sup><italic>¯</italic></sup><italic>, a SG-lightlike submanifold </italic><inline-formula><tex-math id="math-506"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is mixed geodesic </italic><inline-formula><tex-math id="math-507"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle i f \end{document} ]]></tex-math></inline-formula><italic> and only if the following conditions hold</italic></p><disp-formula id="equation-126"><tex-math id="math-508"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle (i) \quad C ^ {\prime} (\bar {h} ^ {\circ^ {l}} (X ^ {\circ}, f ^ {\prime} Z ^ {\circ}) + \bar {D} ^ {\circ^ {l}} (X ^ {\circ}, w ^ {\prime} Z ^ {\circ})) = 0, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-127"><tex-math id="math-509"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle (i i) \quad w ^ {\prime} (\Omega_ {X ^ {\circ}} f ^ {\prime} Z ^ {\circ} - \bar {A} _ {w ^ {\prime} Z ^ {\circ}} X ^ {\circ}) = - C ^ {\prime} (\bar {h} ^ {s} (X ^ {\circ}, f ^ {\prime} Z ^ {\circ}) + \bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {\prime} Z ^ {\circ}), \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-128"><tex-math id="math-510"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle (i i i) \quad \bar {h} ^ {\circ^ {s}} (X ^ {\circ}, f ^ {\prime} Z ^ {\circ}) + \bar {D} ^ {\circ^ {l}} (X ^ {\circ}, w ^ {\prime} Z ^ {\circ}) = - \bar {h} ^ {\circ^ {l}} (X ^ {\circ}, f ^ {\prime} Z ^ {\circ}) - \bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {\prime} Z ^ {\circ}, \end{document} ]]></tex-math></disp-formula><p><italic>for any </italic><inline-formula><tex-math id="math-511"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \in \Gamma ( B ) , ~ Z ^ { \circ } \in \Gamma ( B ^ { ' } ) \end{document} ]]></tex-math></inline-formula></p><p><italic>Proof</italic>. Let <inline-formula><tex-math id="math-512"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> be a mixed geodesic SG-lightlike submanifold.</p><p>From <xref ref-type="disp-formula" rid="equation-6">(1)</xref>, <xref ref-type="disp-formula" rid="equation-20">(13)</xref>, <xref ref-type="disp-formula" rid="equation-30">(22)</xref> and <xref ref-type="disp-formula" rid="equation-31">(23)</xref>, we get</p><disp-formula id="equation-129"><tex-math id="math-513"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & h ^ {\circ} (X ^ {\circ}, Z ^ {\circ}) = \bar {J} ^ {\prime} (\bar {\Omega} _ {X ^ {\circ}} f ^ {'} Z ^ {\circ}) + \bar {J} ^ {\prime} (\bar {\Omega} _ {X ^ {\circ}} w ^ {'} Z ^ {\circ}) + 3 l \theta (\bar {J} ^ {\prime} Z ^ {\circ}) X ^ {\circ} + l \theta (Z ^ {\circ}) X ^ {\circ} \\ & \qquad - l \theta (\bar {J} ^ {\prime} Z ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} + m \theta (Z ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} - m \theta (\bar {J} ^ {\prime} Z ^ {\circ}) X ^ {\circ} \\ & \qquad - 3 \bar {\Omega} _ {X ^ {\circ}} f ^ {'} Z ^ {\circ} - 3 \bar {\Omega} _ {X ^ {\circ}} w ^ {'} Z ^ {\circ} - \Omega_ {X ^ {\circ}} Z ^ {\circ}, \end{array} \end{document} ]]></tex-math></disp-formula><p>Employing <xref ref-type="disp-formula" rid="equation-24">(17)</xref>, <xref ref-type="disp-formula" rid="equation-25">(18)</xref>, <xref ref-type="disp-formula" rid="equation-36">(26)</xref> and <xref ref-type="disp-formula" rid="equation-44">(33)</xref> on above equation and comparing the transversal parts, we obtain</p><disp-formula id="equation-130"><tex-math id="math-514"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & h ^ {\circ} (X ^ {\circ}, Z ^ {\circ}) = w ^ {'} (\Omega_ {X ^ {\circ}} f ^ {'} Z ^ {\circ}) + C ^ {'} (\bar {h ^ {\circ}} ^ {l} (X ^ {\circ}, f ^ {'} Z ^ {\circ})) + C ^ {'} (\bar {h ^ {\circ}} ^ {s} (X ^ {\circ}, f ^ {'} Z ^ {\circ})) \\ & \qquad + w ^ {'} (- \bar {A} _ {w ^ {'} Z ^ {\circ}} X ^ {\circ}) + C ^ {'} (\bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ}) + C ^ {'} (\bar {D ^ {\circ}} ^ {l} (X ^ {\circ}, f ^ {'} Z ^ {\circ})) \\ & \qquad - 3 \bar {h ^ {\circ}} ^ {l} (X ^ {\circ}, f ^ {'} Z ^ {\circ}) - 3 \bar {h ^ {\circ}} ^ {s} (X ^ {\circ}, f ^ {'} Z ^ {\circ}) \\ & \qquad - 3 \bar {\Omega} _ {X ^ {\circ}} ^ {s} w ^ {'} Z ^ {\circ} - 3 \bar {D ^ {\circ}} ^ {l} (X ^ {\circ}, w ^ {'} Z ^ {\circ}) \\ & \qquad = 0. \end{array} \end{document} ]]></tex-math></disp-formula></sec><sec id="sec-6"><title>6. TOTALLY UMBILICAL SG-LIGHTLIKE SUBMANIFOLDS</title><p><bold>Definition 6.1.</bold><xref ref-type="bibr" rid="BIBR-16">[16]</xref><italic> ”Consider a lightlike submanifold </italic><inline-formula><tex-math id="math-515"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( M ^ { \circ } , g ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> ofa semi-Riemannian manifold </italic><inline-formula><tex-math id="math-516"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M } ^ { \circ } , \bar { g } ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> is said to be totally umbilical in </italic><inline-formula><tex-math id="math-517"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { M } } ^ { \circ } { \mathrm { ~ } } i f \end{document} ]]></tex-math></inline-formula><italic> there exist a smooth transversal vector field </italic><inline-formula><tex-math id="math-518"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle H ^ { \circ } \in \Gamma ( l t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula><italic> on </italic><inline-formula><tex-math id="math-519"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } , \end{document} ]]></tex-math></inline-formula><italic> called the transversal curvature vector field of </italic><inline-formula><tex-math id="math-520"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> , such that, for all </italic><inline-formula><tex-math id="math-521"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> ，</italic></p><disp-formula id="equation-131"><tex-math id="math-522"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ {\circ} (X ^ {\circ}, Y ^ {\circ}) = H ^ {\circ} g ^ {^ {\prime}} (X ^ {\circ}, Y ^ {\circ}),\tag{50} \end{document} ]]></tex-math></disp-formula><p>The Gauss and Weingarten equations for <inline-formula><tex-math id="math-523"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> implies that <inline-formula><tex-math id="math-524"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is totally umbilical if and only if on each coordinate neighborhood <inline-formula><tex-math id="math-525"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle U ^ { \circ } \end{document} ]]></tex-math></inline-formula> , there exist smooth vector fields <inline-formula><tex-math id="math-526"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle H ^ { \circ l } \in \Gamma ( l t r ( T M ^ { \circ } ) ) \end{document} ]]></tex-math></inline-formula> ) and <inline-formula><tex-math id="math-527"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle H ^ { \circ s } \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula> ), such that</p><disp-formula id="equation-132"><tex-math id="math-528"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ {\circ l} (X ^ {\circ}, Y ^ {\circ}) = H ^ {\circ l} g ^ {\prime} (X ^ {\circ}, Y ^ {\circ}), h ^ {\circ s} (X ^ {\circ}, Y ^ {\circ}) = H ^ {\circ s} g ^ {\prime} (X ^ {\circ}, Y ^ {\circ}), D ^ {\circ l} (X ^ {\circ}, W ^ {\circ}) = 0,\tag{51} \end{document} ]]></tex-math></disp-formula><p>for all <inline-formula><tex-math id="math-529"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( T M ^ { \circ } ) , W ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula><target id="anchor-1" target-type="reference-target"/></p><p><bold>Lemma 6.2.</bold><italic>Let </italic><inline-formula><tex-math id="math-530"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> be a totally umbilical proper SG-lightlike submanifold of a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-531"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> with an (l, m)-type connection Ω</italic><sup><italic>¯</italic></sup><italic>. Then,</italic></p><disp-formula id="equation-133"><tex-math id="math-532"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}(i)\quad & \Omega_{X^\circ} f'Y^\circ - \bar{A}_{w'_l Y^\circ} X^\circ - \bar{A}_{w'_s Y^\circ} X^\circ - l\theta(J'Y^\circ)X^\circ - m\theta(J'Y^\circ)f'X^\circ \\&= f'\Omega_{X^\circ} Y^\circ + B'\bar{h}^{\circ s}(X^\circ, Y^\circ) - l\theta(Y^\circ)f'X^\circ - 3m\theta(Y^\circ)f'X^\circ - m\theta(Y^\circ)X^\circ, \\[1em](ii)\quad & \bar{h}^{\circ l}(X^\circ, f'Y^\circ) + \bar{\Omega}^{l}_{X^\circ} w'_l Y^\circ - m\theta(J'Y^\circ) w'_l X^\circ \\&= w'_l \Omega_{X^\circ} Y^\circ + C'\bar{h}^{\circ l}(X^\circ, Y^\circ) - l\theta(Y^\circ) w'_l X^\circ - 3m\theta(Y^\circ) w'_l X^\circ, \\[1em](iii)\quad & \bar{h}^{\circ s}(X^\circ, f'Y^\circ) + \bar{D}^{\circ s}(X^\circ, w'_l Y^\circ) + \bar{\Omega}^{s}_{X^\circ} w'_s Y^\circ - m\theta(J'Y^\circ) w'_s X^\circ \\&= w'_s \Omega_{X^\circ} Y^\circ + C'\bar{h}^{\circ s}(X^\circ, Y^\circ) - l\theta(Y^\circ) w'_s X^\circ - 3m\theta(Y^\circ) w'_s X^\circ,\end{align*} \end{document} ]]></tex-math></disp-formula><p><italic>for any </italic><inline-formula><tex-math id="math-533"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } , Y ^ { \circ } \in \Gamma ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula></p><p><italic>Proof</italic>. Since <inline-formula><tex-math id="math-534"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> is a locally bronze semi-Riemannian manifold, it implies that <inline-formula><tex-math id="math-535"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \nabla } _ { X ^ { \circ } } ^ { \circ } \bar { J } ^ { \prime } Y ^ { \circ } = \bar { J } ^ { \prime } ( \bar { \nabla } _ { X ^ { \circ } } ^ { \circ } Y ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> ,</p><p>Following equation <xref ref-type="disp-formula" rid="equation-31">(23)</xref>, we obtain</p><disp-formula id="equation-134"><tex-math id="math-536"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\Omega} _ {X ^ {\circ}} \bar {J} ^ {\prime} Y ^ {\circ} - l \theta (\bar {J} ^ {\prime} Y ^ {\circ}) X ^ {\circ} - m \theta (\bar {J} ^ {\prime} Y ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} = \bar {J} ^ {\prime} (\bar {\Omega} _ {X ^ {\circ}} Y ^ {\circ}) - l \theta (Y ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} - m \theta (Y ^ {\circ}) \bar {J} ^ {2} X ^ {\circ}, \end{document} ]]></tex-math></disp-formula><p>Using equations <xref ref-type="disp-formula" rid="equation-20">(13)</xref>, <xref ref-type="disp-formula" rid="equation-24">(17)</xref> and <xref ref-type="disp-formula" rid="equation-25">(18)</xref>, we get</p><disp-formula id="equation-135"><tex-math id="math-537"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {\bar {\Omega} _ {X ^ {\circ}} f ^ {'} Y ^ {\circ} + \bar {\Omega} _ {X ^ {\circ}} w _ {l} ^ {'} Y ^ {\circ} + \bar {\Omega} _ {X ^ {\circ}} w _ {s} ^ {'} Y ^ {\circ} - l \theta (\bar {J} ^ {'} Y ^ {\circ}) X ^ {\circ}} \\ & {- m \theta (\bar {J} ^ {'} Y ^ {\circ}) f ^ {'} X ^ {\circ} - m \theta (\bar {J} ^ {'} Y ^ {\circ}) w _ {l} ^ {'} X ^ {\circ} - m \theta (\bar {J} ^ {'} Y ^ {\circ}) w _ {s} ^ {'} X ^ {\circ}} \\ & {= \bar {J} ^ {'} (\bar {\Omega} _ {X ^ {\circ}} Y ^ {\circ}) - l \theta (Y ^ {\circ}) f ^ {'} X ^ {\circ} - l \theta (Y ^ {\circ}) w _ {l} ^ {'} X ^ {\circ} - l \theta (Y ^ {\circ}) w _ {s} ^ {'} X ^ {\circ}} \\ & {- 3 m \theta (Y ^ {\circ}) f ^ {'} X ^ {\circ} - 3 m \theta (Y ^ {\circ}) w _ {l} ^ {'} X ^ {\circ} - 3 m \theta (Y ^ {\circ}) w _ {s} ^ {'} X ^ {\circ} - m \theta (Y ^ {\circ}) X ^ {\circ},} \end{array} \end{document} ]]></tex-math></disp-formula><p>From equations <xref ref-type="disp-formula" rid="equation-36">(26)</xref>, <xref ref-type="disp-formula" rid="equation-43">(32)</xref>, <xref ref-type="disp-formula" rid="equation-44">(33)</xref> and <xref ref-type="disp-formula" rid="equation-132">(51)</xref>, we attain</p><disp-formula id="equation-136"><tex-math id="math-538"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {\Omega_ {X ^ {\circ}} f ^ {'} Y ^ {\circ} + \bar {h} ^ {\circ^ {l}} (X ^ {\circ}, f ^ {'} Y ^ {\circ}) + \bar {h} ^ {\circ^ {s}} (X ^ {\circ}, f ^ {'} Y ^ {\circ}) - \bar {A} _ {w _ {l} ^ {'} Y ^ {\circ}} X ^ {\circ} + \bar {\Omega} _ {X ^ {\circ}} ^ {l} w _ {l} ^ {'} Y ^ {\circ}} \\ & {\qquad + \bar {D} ^ {\circ^ {s}} (X ^ {\circ}, w _ {l} ^ {'} Y ^ {\circ}) - \bar {A} _ {w _ {s} ^ {'} Y ^ {\circ}} X ^ {\circ} + \bar {\Omega} _ {X ^ {\circ}} ^ {l} w _ {s} ^ {'} Y ^ {\circ} - l \theta (\bar {J} ^ {'} Y ^ {\circ}) X ^ {\circ}} \\ & {\qquad - m \theta (\bar {J} ^ {'} Y ^ {\circ}) f ^ {'} X ^ {\circ} - m \theta (\bar {J} ^ {'} Y ^ {\circ}) w _ {l} ^ {'} X ^ {\circ} - m \theta (\bar {J} ^ {'} Y ^ {\circ}) w _ {s} ^ {'} X ^ {\circ}} \\ & {\qquad = f ^ {'} \Omega_ {X ^ {\circ}} Y ^ {\circ} + w _ {l} ^ {'} \Omega_ {X ^ {\circ}} Y ^ {\circ} + w _ {s} ^ {'} \Omega_ {X ^ {\circ}} Y ^ {\circ} + C ^ {'} \bar {h} ^ {\circ^ {l}} (X ^ {\circ}, Y ^ {\circ})} \\ & {\qquad + B ^ {'} \bar {h} ^ {\circ^ {s}} (X ^ {\circ}, Y ^ {\circ}) + C ^ {'} \bar {h} ^ {\circ^ {s}} (X ^ {\circ}, Y ^ {\circ}) - l \theta (Y ^ {\circ}) f ^ {'} X ^ {\circ} - l \theta (Y ^ {\circ}) w _ {l} ^ {'} X ^ {\circ}} \\ & {\qquad - l \theta (Y ^ {\circ}) w _ {s} ^ {'} X ^ {\circ} - 3 m \theta (Y ^ {\circ}) f ^ {'} X ^ {\circ} - 3 m \theta (Y ^ {\circ}) w _ {l} ^ {'} X ^ {\circ} - 3 m \theta (Y ^ {\circ}) w _ {s} ^ {'} X ^ {\circ}} \\ & {\qquad - m \theta (Y ^ {\circ}) X ^ {\circ},} \end{array} \end{document} ]]></tex-math></disp-formula><p>Thus the required result is obtained by comparing the tangential and normal parts of above equation. □</p><p><bold>Theorem 6.3.</bold><italic>If </italic><inline-formula><tex-math id="math-539"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is a totally umbilical proper SG-lightlike submanifold of a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-540"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> with an </italic><inline-formula><tex-math id="math-541"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) { - } t y p e \end{document} ]]></tex-math></inline-formula><italic> connection Ω</italic><sup><italic>¯</italic></sup><italic>, then </italic><inline-formula><tex-math id="math-542"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle H ^ { \circ s } \notin \Gamma ( \mu ^ { \circ } ). \end{document} ]]></tex-math></inline-formula></p><p><italic>Proof</italic>. Let <inline-formula><tex-math id="math-543"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> be a totally umbilical proper SG-lightlike submanifold of a locally bronze semi-Riemannian manifold, then <inline-formula><tex-math id="math-544"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \nabla } _ { X ^ { \circ } } ^ { \circ } \bar { J ^ { \prime } } Y ^ { \circ } = \bar { J ^ { \prime } } ( \bar { \nabla } _ { X ^ { \circ } } ^ { \circ } Y ^ { \circ } ) \end{document} ]]></tex-math></inline-formula></p><p>Now, using equations <xref ref-type="disp-formula" rid="equation-20">(13)</xref>, <xref ref-type="disp-formula" rid="equation-24">(17)</xref>, <xref ref-type="disp-formula" rid="equation-25">(18)</xref>, <xref ref-type="disp-formula" rid="equation-31">(23)</xref>, <xref ref-type="disp-formula" rid="equation-36">(26)</xref> and comparing transversal parts, we obtain</p><disp-formula id="equation-137"><tex-math id="math-545"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ {\circ s} (X ^ {\circ}, \bar {J} ^ {\prime} X ^ {\circ}) + m \theta (\bar {J} ^ {\prime} X ^ {\circ}) w _ {s} ^ {\prime} X ^ {\circ} = C ^ {\prime} h ^ {\circ s} (X ^ {\circ}, X ^ {\circ}) + C ^ {\prime} m \theta (X ^ {\circ}) w _ {s} ^ {\prime} X ^ {\circ}, \forall X ^ {\circ}, Y ^ {\circ} \in \end{document} ]]></tex-math></disp-formula><p>From the concept of totally umbilical submanifold <inline-formula><tex-math id="math-546"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> of <inline-formula><tex-math id="math-547"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> , we get</p><disp-formula id="equation-138"><tex-math id="math-548"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle g ^ {\prime} (X ^ {\circ}, \bar {J} ^ {\prime} X ^ {\circ}) H ^ {\circ s} + m \theta (\bar {J} ^ {\prime} X ^ {\circ}) w _ {s} ^ {\prime} X ^ {\circ} = g ^ {\prime} (X ^ {\circ}, X ^ {\circ}) C ^ {\prime} H ^ {\circ s} + C ^ {\prime} m \theta (\bar {X} ^ {\circ}) w _ {s} ^ {\prime} X ^ {\circ}, \end{document} ]]></tex-math></disp-formula><p>Since <inline-formula><tex-math id="math-549"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is a SG-lightlike submanifold of <inline-formula><tex-math id="math-550"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> , it is inferred that the distribution B is invariant with respect to <inline-formula><tex-math id="math-551"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } } ^ { \prime } \end{document} ]]></tex-math></inline-formula> . Also, if we take <inline-formula><tex-math id="math-552"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } = Y ^ { \circ } \end{document} ]]></tex-math></inline-formula> , then <inline-formula><tex-math id="math-553"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle g ^ { ' } ( X ^ { \circ } , X ^ { \circ } ) C ^ { ' } H ^ { \circ s } = \end{document} ]]></tex-math></inline-formula><inline-formula><tex-math id="math-554"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle 0 , \ w _ { s } ^ { ' } X ^ { \circ } = 0 \end{document} ]]></tex-math></inline-formula></p><p>Hence, <inline-formula><tex-math id="math-555"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle H ^ { \circ s } \notin \Gamma ( \mu ^ { \circ } ) \end{document} ]]></tex-math></inline-formula></p><p><bold>Theorem 6.4.</bold><italic>Let </italic><inline-formula><tex-math id="math-556"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> be a totally umbilical proper SG-lightlike submanifold of a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-557"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> with an </italic><inline-formula><tex-math id="math-558"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula><italic> -type connection Ω</italic><sup><italic>¯</italic></sup><italic>. Then the necessary and suficient condition for induced connection to be metric is </italic><inline-formula><tex-math id="math-559"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle l \theta ( Y ^ { \circ } ) g ^ { ' } ( X ^ { \circ } , Z ^ { \circ } ) + m \theta ( Y ^ { \circ } ) g ^ { ' } ( f ^ { ' } X ^ { \circ } , Z ^ { \circ } ) = - l \theta ( Z ^ { \circ } ) g ^ { ' } ( Y ^ { \circ } , X ^ { \circ } ) - m \theta ( Z ^ { \circ } ) g ^ { ' } ( Y ^ { \circ } , f ^ { ' } Z ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic></italic><inline-formula><tex-math id="math-560"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \forall X ^ { \circ } , Y ^ { \circ } , Z ^ { \circ } \in \Gamma ( B _ { o } ) \end{document} ]]></tex-math></inline-formula></p><p><italic>Proof</italic>. Lemma (<xref ref-type="custom" custom-type="reference-target" rid="anchor-1">6.2</xref>) implies</p><disp-formula id="equation-139"><tex-math id="math-561"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {h} ^ {\circ l} (X ^ {\circ}, f ^ {\prime} Y ^ {\circ}) + \bar {\Omega} _ {X ^ {\circ}} ^ {l} w _ {l} ^ {\prime} Y ^ {\circ} - m \theta (\bar {J} ^ {\prime} Y ^ {\circ}) w _ {l} ^ {\prime} X ^ {\circ} = w _ {l} ^ {\prime} \Omega_ {X ^ {\circ}} Y ^ {\circ} + C ^ {\prime} \bar {h} ^ {\circ l} (X ^ {\circ}, Y ^ {\circ}) - l \theta (Y ^ {\circ}) w _ {l} ^ {\prime} X ^ {\circ} - \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-140"><tex-math id="math-562"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle 3 m \theta (Y ^ {\circ}) w _ {l} ^ {\prime} X ^ {\circ} \end{document} ]]></tex-math></disp-formula><p>Since <inline-formula><tex-math id="math-563"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is a totally umbillical proper SG-lightlike submanifold, therefore</p><disp-formula id="equation-141"><tex-math id="math-564"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ {\circ l} \left(X ^ {\circ}, \bar {J} ^ {\prime} Y ^ {\circ}\right) + m \theta \left(\bar {J} ^ {\prime} Y ^ {\circ}\right) w _ {l} ^ {\prime} X ^ {\circ} = C ^ {\prime} h ^ {\circ l} \left(X ^ {\circ}, Y ^ {\circ}\right) + C ^ {\prime} m \theta \left(Y ^ {\circ}\right) w _ {l} ^ {\prime} X ^ {\circ}, \end{document} ]]></tex-math></disp-formula><p>Since the distribution <inline-formula><tex-math id="math-565"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } \end{document} ]]></tex-math></inline-formula> is invariant with respect to bronze structure <inline-formula><tex-math id="math-566"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } ^ { \prime } } . \end{document} ]]></tex-math></inline-formula> , we have <inline-formula><tex-math id="math-567"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle w _ { l } ^ { ' } X ^ { \circ } = 0 \end{document} ]]></tex-math></inline-formula> . Also, from equations <xref ref-type="disp-formula" rid="equation-131">(50)</xref> and <xref ref-type="disp-formula" rid="equation-132">(51)</xref>, we attain</p><p><inline-formula><tex-math id="math-568"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle g ^ { ' } ( X ^ { \circ } , \bar { J } ^ { \prime } Y ^ { \circ } ) H ^ { \circ l } = g ^ { ' } ( X ^ { \circ } , Y ^ { \circ } ) C ^ { ' } H ^ { \circ l } \end{document} ]]></tex-math></inline-formula> , which leads to <inline-formula><tex-math id="math-569"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle 2 g ^ { ' } ( X ^ { \circ } , \bar { J } ^ { \prime } Y ^ { \circ } ) H ^ { \circ l } = 0 \end{document} ]]></tex-math></inline-formula></p><p>If we take <inline-formula><tex-math id="math-570"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } = { \bar { J } } ^ { \prime } Y ^ { \circ } \end{document} ]]></tex-math></inline-formula> , then <inline-formula><tex-math id="math-571"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle H ^ { \circ l } = 0 ; \end{document} ]]></tex-math></inline-formula> , so equation <xref ref-type="disp-formula" rid="equation-132">(51)</xref> implies that <inline-formula><tex-math id="math-572"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ { \circ l } = 0, \end{document} ]]></tex-math></inline-formula></p><p>Employing equation <xref ref-type="disp-formula" rid="equation-40">(30)</xref>, we have</p><disp-formula id="equation-142"><tex-math id="math-573"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \left(\Omega_ {X ^ {\circ}} g ^ {\prime}\right) \left(Y ^ {\circ}, Z ^ {\circ}\right) = - l \left(\theta \left(Y ^ {\circ}\right) g ^ {\prime} \left(X ^ {\circ}, Z ^ {\circ}\right) + \theta \left(Z ^ {\circ}\right) g ^ {\prime} \left(Y ^ {\circ}, X ^ {\circ}\right)\right) - m \left(\theta \left(Y ^ {\circ}\right) g ^ {\prime} \left(f ^ {\prime} X ^ {\circ}, Z ^ {\circ}\right) + \right. \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-143"><tex-math id="math-574"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \theta (Z ^ {\circ}) g ^ {\prime} \left(Y ^ {\circ}, f ^ {\prime} Z ^ {\circ}\right)) = 0. \end{document} ]]></tex-math></disp-formula></sec><sec id="sec-7"><title>7. MINIMAL SG-LIGHTLIKE SUBMANIFOLDS</title><p><bold>Definition 7.1.</bold><italic></italic><xref ref-type="bibr" rid="BIBR-17">[17]</xref><italic> A lightlike submanifold </italic><inline-formula><tex-math id="math-575"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( M ^ { \circ } , g ^ { ' } , S ( T M ^ { \circ } ) , S ( T M ^ { \circ \bot } ) ) \end{document} ]]></tex-math></inline-formula><italic> , of a semi-Riemannian manifold </italic><inline-formula><tex-math id="math-576"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M } ^ { \circ } , \bar { g } ^ { ' } ) \end{document} ]]></tex-math></inline-formula><italic> , is said to be minimal </italic><inline-formula><tex-math id="math-577"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle i f \end{document} ]]></tex-math></inline-formula><italic> :</italic></p><p><italic>(i) </italic><inline-formula><tex-math id="math-578"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ { \circ s } = 0 \end{document} ]]></tex-math></inline-formula><italic> on </italic><inline-formula><tex-math id="math-579"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle R a d ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> and</italic></p><p><italic>(ii) trace </italic><inline-formula><tex-math id="math-580"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ { \circ } = 0 \end{document} ]]></tex-math></inline-formula><italic> , where trace is written with respect to </italic><inline-formula><tex-math id="math-581"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle g ^ { ' } \end{document} ]]></tex-math></inline-formula><italic> restricted to </italic><inline-formula><tex-math id="math-582"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula></p><p>The above definition is independent of <inline-formula><tex-math id="math-583"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-584"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) \end{document} ]]></tex-math></inline-formula> ), but is dependent on <inline-formula><tex-math id="math-585"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> .</p><p><bold>Example 7.2.</bold><italic>let </italic><inline-formula><tex-math id="math-586"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } = \mathbb { R } _ { 1 } ^ { 1 1 } \end{document} ]]></tex-math></inline-formula><italic> be a semi-Riemannian space of signature </italic><inline-formula><tex-math id="math-587"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( - , + , + , + , + , + , + , + , + , + , + , + ) \end{document} ]]></tex-math></inline-formula><italic> , with canonical basis</italic></p><disp-formula id="equation-144"><tex-math id="math-588"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{\partial y _ {1} ^ {\circ}, \partial y _ {2} ^ {\circ}, \partial y _ {3} ^ {\circ}, \partial y _ {4} ^ {\circ}, \partial y _ {5} ^ {\circ}, \partial y _ {6} ^ {\circ}, \partial y _ {7} ^ {\circ}, \partial y _ {8} ^ {\circ}, \partial y _ {9} ^ {\circ}, \partial y _ {1 0} ^ {\circ}, \partial y _ {1 1} ^ {\circ} \}. \end{document} ]]></tex-math></disp-formula><p><italic>Let </italic><inline-formula><tex-math id="math-589"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> be a submanifold </italic><inline-formula><tex-math id="math-590"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle o f \left( \mathbb { R } _ { 1 } ^ { 1 1 } , \bar { J } ^ { \prime } \right) \end{document} ]]></tex-math></inline-formula><italic> given by</italic></p><disp-formula id="equation-145"><tex-math id="math-591"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}y_1^\circ &= 0, \quad y_2^\circ = \frac{1}{2}(\sqrt{3}\,t_4' + t_2'), \\[1em]y_3^\circ &= \frac{1}{2}(-\sqrt{3}\,t_2' + t_4'), \quad y_4^\circ = t_1', \quad y_5^\circ = t_4', \\[1em]y_6^\circ &= \sin t_5' \sinh t_6', \quad y_7^\circ = 0, \quad y_8^\circ = \sin t_5' \cosh t_6', \\[1em]y_9^\circ &= 0, \quad y_{10}^\circ = \sqrt{2}\cos t_5' \cosh t_6', \quad y_{11}^\circ = 0.\end{align*} \end{document} ]]></tex-math></disp-formula><p><italic>Consider the bronze structure </italic><sup><italic>¯</italic></sup><italic>J</italic><sup><italic>′</italic></sup><italic> defined by </italic><inline-formula><tex-math id="math-592"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } ( y _ { 1 } ^ { \circ } , y _ { 2 } ^ { \circ } , y _ { 3 } ^ { \circ } , y _ { 4 } ^ { \circ } , y _ { 5 } ^ { \circ } , y _ { 6 } ^ { \circ } , y _ { 7 } ^ { \circ } , y _ { 8 } ^ { \circ } , y _ { 9 } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic></italic><inline-formula><tex-math id="math-593"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle y _ { 1 0 } ^ { \circ } , y _ { 1 1 } ^ { \circ } ) = ( \omega y _ { 1 } ^ { \circ } , ( 3 - \omega ) y _ { 2 } ^ { \circ } , ( 3 - \omega ) y _ { 3 } ^ { \circ } , \omega y _ { 4 } ^ { \circ } , ( 3 - \omega ) y _ { 5 } ^ { \circ } , 3 y _ { 6 } ^ { \circ } + y _ { 7 } ^ { \circ } , y _ { 6 } ^ { \circ } , 3 y _ { 8 } ^ { \circ } + y _ { 9 } ^ { \circ } , y _ { 8 } ^ { \circ } , 3 y _ { 1 0 } ^ { \circ } + y _ { 1 1 } ^ { \circ } , y _ { 1 2 } ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><inline-formula><tex-math id="math-594"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle y _ { 1 1 } ^ { \circ } , y _ { 1 0 } ^ { \circ } ). \end{document} ]]></tex-math></inline-formula></p><p><italic>Then, </italic><inline-formula><tex-math id="math-595"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle T M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> is spanned by </italic><inline-formula><tex-math id="math-596"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ B _ { 1 } , B _ { 2 } , B _ { 3 } , B _ { 4 } , B _ { 5 } \} \end{document} ]]></tex-math></inline-formula><italic> , where</italic></p><disp-formula id="equation-146"><tex-math id="math-597"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}B_1 &= \frac{1}{2}\left(-\sqrt{3}\,\partial y_3^\circ + \partial y_2^\circ\right), \\B_2 &= \partial y_4^\circ, \\B_3 &= \partial y_5^\circ + \frac{1}{2}\left(\sqrt{3}\,\partial y_2^\circ + \partial y_3^\circ\right), \\B_4 &= \cos t_5' \sinh t_6' \,\partial y_6^\circ + \cos t_5' \cosh t_6' \,\partial y_8^\circ - \sqrt{2}\sin t_5' \cosh t_6' \,\partial y_{10}^\circ, \\B_5 &= \sin t_5' \cosh t_6' \,\partial y_6^\circ + \sin t_5' \sinh t_6' \,\partial y_8^\circ + \sqrt{2}\cos t_5' \sinh t_6' \,\partial y_{10}^\circ.\end{align*} \end{document} ]]></tex-math></disp-formula><p><italic>where </italic><inline-formula><tex-math id="math-598"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle R a d ( T M ^ { \circ } ) = S p a n \{ B _ { 3 } \} \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-599"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } = S p a n \{ B _ { 1 } , B _ { 2 } \} \end{document} ]]></tex-math></inline-formula><italic> . It is proved that </italic><inline-formula><tex-math id="math-600"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } B _ { 3 } = ( 3 - \omega ) \dot { B } _ { 3 } \end{document} ]]></tex-math></inline-formula><italic> , which shows that Rad(TM</italic><sup><italic>◦</italic></sup><italic>) is invariant under </italic><inline-formula><tex-math id="math-601"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { \boldsymbol { J } } ^ { \prime } \end{document} ]]></tex-math></inline-formula><italic> . Since, </italic><inline-formula><tex-math id="math-602"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } B _ { 1 } = ( 3 - \omega ) B _ { 1 } , \bar { J } ^ { \prime } B _ { 2 } = \omega B _ { 1 } \end{document} ]]></tex-math></inline-formula><italic> . Therefore, </italic><inline-formula><tex-math id="math-603"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } = S p a n \{ B _ { 1 } , B _ { 2 } \} \end{document} ]]></tex-math></inline-formula><italic> , is invariant under </italic><sup><italic>¯</italic></sup><italic>J</italic><sup><italic>′</italic></sup><italic>.</italic></p><p><italic>Upon calculation, we derive that </italic><inline-formula><tex-math id="math-604"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle l t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> is spanned by</italic></p><disp-formula id="equation-147"><tex-math id="math-605"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle N = \frac {1}{2} \{- \partial y _ {5} ^ {\circ} + \frac {1}{2} \partial y _ {3} ^ {\circ} + \frac {\sqrt {3}}{2} \partial y _ {2} ^ {\circ} \}, \end{document} ]]></tex-math></disp-formula><p><italic>such that </italic><inline-formula><tex-math id="math-606"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } N = ( 3 - \omega ) N \end{document} ]]></tex-math></inline-formula><italic> , which implies that </italic><inline-formula><tex-math id="math-607"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle l t r ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> is invariant under </italic><inline-formula><tex-math id="math-608"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } ^ { \prime } } \end{document} ]]></tex-math></inline-formula><italic></italic><inline-formula><tex-math id="math-609"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle A l s o , S ( T M ^ { \circ \bot } ) \end{document} ]]></tex-math></inline-formula><italic> is spanned by</italic></p><disp-formula id="equation-148"><tex-math id="math-610"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}W_1 &= \partial y_1^\circ, \\W_2 &= \cos t_5' \sinh t_6' \,\partial y_7^\circ + \cos t_5' \cosh t_6' \,\partial y_9^\circ - \sqrt{2}\sin t_5' \cosh t_6' \,\partial y_{11}^\circ, \\W_3 &= \sin t_5' \cosh t_6' \,\partial y_7^\circ + \sin t_5' \sinh t_6' \,\partial y_9^\circ + \sqrt{2}\cos t_5' \sinh t_6' \,\partial y_{11}^\circ, \\W_4 &= -\sqrt{2}\sinh t_6' \cosh t_6' \,\partial y_7^\circ + \sqrt{2}\left(\sin^2 t_5' + \sinh^2 t_6'\right)\partial y_9^\circ + \sin t_5' \cos t_5' \,\partial y_{11}^\circ, \\W_5 &= -\sqrt{2}\sinh t_6' \cosh t_6' \,\partial y_6^\circ + \sqrt{2}\left(\sin^2 t_5' + \sinh^2 t_6'\right)\partial y_8^\circ + \sin t_5' \cos t_5' \,\partial y_{10}^\circ.\end{align*} \end{document} ]]></tex-math></disp-formula><p><italic>Since, </italic><inline-formula><tex-math id="math-611"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } W _ { 4 } = W _ { 5 } , \bar { J } ^ { \prime } W _ { 5 } = 3 W _ { 5 } + W _ { 4 } \end{document} ]]></tex-math></inline-formula><italic> , we see that </italic><inline-formula><tex-math id="math-612"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \mu ^ { \circ } = S p a n \{ W _ { 4 } , W _ { 5 } \} \end{document} ]]></tex-math></inline-formula><italic> is invariant under </italic><inline-formula><tex-math id="math-613"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } ^ { \prime } } \end{document} ]]></tex-math></inline-formula><italic> . Now, </italic><inline-formula><tex-math id="math-614"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B ^ { ' } = S p a n \{ B _ { 4 } , B _ { 5 } \} \end{document} ]]></tex-math></inline-formula><italic> such that </italic><inline-formula><tex-math id="math-615"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } B _ { 4 } = 3 B _ { 4 } + W _ { 2 } \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-616"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } B _ { 5 } = \end{document} ]]></tex-math></inline-formula><italic></italic><inline-formula><tex-math id="math-617"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle 3 B _ { 5 } + W _ { 3 } \end{document} ]]></tex-math></inline-formula><italic> , which shows that </italic><inline-formula><tex-math id="math-618"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J } ^ { \prime } ( B ^ { ' } ) \subset S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> and </italic><inline-formula><tex-math id="math-619"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { J ^ { \prime } } ( B ^ { ' } ) \subset S ( T M ^ { \circ \bot } ) \end{document} ]]></tex-math></inline-formula><italic> . Therefore. M° is a proper SG-1-lightlike submanifold of </italic><inline-formula><tex-math id="math-620"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \mathbb{R}_1^{11}. \end{document} ]]></tex-math></inline-formula></p><p><italic>Also, we derive upon calculation</italic></p><disp-formula id="equation-149"><tex-math id="math-621"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar {\nabla} _ {B _ {i}} ^ {\circ} B _ {j} = 0, i = 1, 2, 3, 1 \leq j \leq 5, a n d h ^ {\circ l} (B _ {4}, B _ {4}) = 0, h ^ {\circ l} (B _ {5}, B _ {5}) = 0, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-150"><tex-math id="math-622"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ {\circ s} (B _ {4}, B _ {4}) = - \frac {\sqrt {2} s i n t _ {5} ^ {\prime} c o s h t _ {6} ^ {\prime}}{(s i n ^ {2} t _ {5} ^ {\prime} + 2 s i n h ^ {2} t _ {6} ^ {\prime}) (1 + s i n ^ {2} t _ {5} ^ {\prime} + 2 s i n h ^ {2} t _ {6} ^ {\prime})} W _ {5}, \end{document} ]]></tex-math></disp-formula><disp-formula id="equation-151"><tex-math id="math-623"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ {\circ s} (B _ {5}, B _ {5}) = \frac {\sqrt {2} s i n t _ {5} ^ {\prime} c o s h t _ {6} ^ {\prime}}{(s i n ^ {2} t _ {5} ^ {\prime} + 2 s i n h ^ {2} t _ {6} ^ {\prime}) (1 + s i n ^ {2} t _ {5} ^ {\prime} + 2 s i n h ^ {2} t _ {6} ^ {\prime})} W _ {5}, \end{document} ]]></tex-math></disp-formula><p><italic>Hence, for all </italic><inline-formula><tex-math id="math-624"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \in \Gamma ( T M ^ { \circ } ) , h ^ { \circ s } ( X ^ { \circ } , B _ { 3 } ) = 0 \end{document} ]]></tex-math></inline-formula></p><p><italic>That is </italic><inline-formula><tex-math id="math-625"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle h ^ { \circ s } = 0 \end{document} ]]></tex-math></inline-formula><italic> on </italic><inline-formula><tex-math id="math-626"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle R a d ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula><italic> and traceh </italic><inline-formula><tex-math id="math-627"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ^ { \circ } | _ { S ( T M ^ { \circ } ) } = h ^ { \circ } ( B _ { 4 } , B _ { 4 } ) + h ^ { \circ } { } ^ { s } ( B _ { 5 } , B _ { 5 } ) = \end{document} ]]></tex-math></inline-formula><italic> 0.</italic></p><p><italic>Therefore, M</italic><sup><italic>◦</italic></sup><italic> is minimal proper SG-lightlike submanifold of </italic><inline-formula><tex-math id="math-628"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \mathbb { R } _ { 1 } ^ { 1 1 }. \end{document} ]]></tex-math></inline-formula></p><p><bold>Theorem 7.3.</bold><italic>The distribution </italic><inline-formula><tex-math id="math-629"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } \end{document} ]]></tex-math></inline-formula><italic> in a SG-lightlike submanifold </italic><inline-formula><tex-math id="math-630"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> of a locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-631"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( \bar { M } ^ { \circ } , \bar { g } ^ { ' } , \bar { J } ^ { \prime } ) \end{document} ]]></tex-math></inline-formula><italic> with an </italic><inline-formula><tex-math id="math-632"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) \end{document} ]]></tex-math></inline-formula><italic> -type connection Ω</italic><sup><italic>¯</italic></sup><italic> is minimal if and only if</italic></p><disp-formula id="equation-152"><tex-math id="math-633"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & 3 \{g ^ {'} (f ^ {'} X ^ {\circ}, \bar {A} _ {W ^ {\circ}} f ^ {'} X ^ {\circ}) + l \theta (W ^ {\circ}) g ^ {'} (X ^ {\circ}, f ^ {' 2} X ^ {\circ}) + m \theta (W ^ {\circ}) g ^ {'} (f ^ {'} X ^ {\circ}, f ^ {' 2} X ^ {\circ}) \} \\ & \qquad = - 2 \{g ^ {'} (\bar {A} _ {W ^ {\circ}} f ^ {'} X ^ {\circ}, X ^ {\circ}) + l \theta (W ^ {\circ}) g ^ {'} (X ^ {\circ}, f ^ {'} X ^ {\circ}) + m \theta (W ^ {\circ}) g ^ {'} (X ^ {\circ}, f ^ {' 2} X ^ {\circ}) \}, \end{array} \end{document} ]]></tex-math></disp-formula><p>for any <inline-formula><tex-math id="math-634"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \in \Gamma ( B _ { o } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-635"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula> .</p><p><italic>Proof</italic>. <inline-formula><tex-math id="math-636"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } \end{document} ]]></tex-math></inline-formula> is minimal if and only if</p><disp-formula id="equation-153"><tex-math id="math-637"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {\Omega_ {X ^ {\circ}} X ^ {\circ} + \Omega_ {\bar {J} ^ {\prime} X ^ {\circ}} \bar {J} ^ {\prime} X ^ {\circ} - l \{\theta (X ^ {\circ}) X ^ {\circ} + \theta (\bar {J} ^ {\prime} X ^ {\circ}) \bar {J} ^ {\prime} X ^ {\circ} \}} \\ & {- m \{\theta (X ^ {\circ}) f ^ {'} X ^ {\circ} + \theta (\bar {J} ^ {\prime} X ^ {\circ}) f ^ {' 2} X ^ {\circ} \} \in \Gamma (B _ {o}),} \end{array}\tag{52} \end{document} ]]></tex-math></disp-formula><p>for all <inline-formula><tex-math id="math-638"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \in \Gamma ( B _ { o } ). \end{document} ]]></tex-math></inline-formula></p><p>Since <inline-formula><tex-math id="math-639"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> is a SG-lightlike submanifold of <inline-formula><tex-math id="math-640"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula> . Therefore, the distribution <inline-formula><tex-math id="math-641"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle B _ { o } \end{document} ]]></tex-math></inline-formula> is invariant w.r.t <inline-formula><tex-math id="math-642"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { J } } ^ { \prime } \end{document} ]]></tex-math></inline-formula> . Also using equations <xref ref-type="disp-formula" rid="equation-37">(27)</xref>, <xref ref-type="disp-formula" rid="equation-8">(3)</xref>, <xref ref-type="disp-formula" rid="equation-23">(16)</xref>, <xref ref-type="disp-formula" rid="equation-21">(14)</xref>, <xref ref-type="disp-formula" rid="equation-10">(5)</xref> and <xref ref-type="disp-formula" rid="equation-47">(36)</xref>, we get</p><disp-formula id="equation-154"><tex-math id="math-643"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & g ^ {'} (\Omega_ {X ^ {\circ}} X ^ {\circ}, \bar {J} ^ {\prime} W ^ {\circ}) - l \theta (X ^ {\circ}) g ^ {'} (X ^ {\circ}, \bar {J} ^ {\prime} W ^ {\circ}) - m \theta (X ^ {\circ}) g ^ {'} (f ^ {'} X ^ {\circ}, \bar {J} ^ {\prime} W ^ {\circ}) \\ & \qquad = g ^ {'} (\bar {J} ^ {\prime} X ^ {\circ}, \bar {A} _ {W ^ {\circ}} X ^ {\circ}) + l \theta (W ^ {\circ}) g ^ {'} (X ^ {\circ}, \bar {J} ^ {\prime} X ^ {\circ}) + m \theta (W ^ {\circ}) g ^ {'} (\bar {J} ^ {\prime} X ^ {\circ}, f ^ {'} X ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p>and</p><disp-formula id="equation-155"><tex-math id="math-644"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & g ^ {'} (\Omega_ {\bar {J} ^ {\prime} X ^ {\circ}} \bar {J} ^ {\prime} X ^ {\circ}, \bar {J} ^ {\prime} W ^ {\circ}) - l \theta (\bar {J} ^ {\prime} X ^ {\circ}) g ^ {'} (\bar {J} ^ {\prime} X ^ {\circ}, \bar {J} ^ {\prime} W ^ {\circ}) - m \theta (\bar {J} ^ {\prime} X ^ {\circ}) g ^ {'} (f ^ {' 2} X ^ {\circ}, \bar {J} ^ {\prime} W ^ {\circ}) \\ & \qquad = g ^ {'} (3 \bar {J} ^ {\prime} X ^ {\circ} + X ^ {\circ}, \bar {A} _ {W ^ {\circ}} \bar {J} ^ {\prime} X ^ {\circ}) + l \theta (W ^ {\circ}) g ^ {'} (3 \bar {J} ^ {\prime} X ^ {\circ} + X ^ {\circ}, \bar {J} ^ {\prime} X ^ {\circ}) \\ & \qquad + m \theta (W ^ {\circ}) g ^ {'} (3 \bar {J} ^ {\prime} X ^ {\circ} + X ^ {\circ}, f ^ {' 2} X ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p>for any <inline-formula><tex-math id="math-645"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \in \Gamma ( B _ { o } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-646"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula></p><p>Also, since the shape operator is symmetric on <inline-formula><tex-math id="math-647"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> , we obtain</p><disp-formula id="equation-156"><tex-math id="math-648"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & g ^ {'} \big (\Omega_ {X ^ {\circ}} X ^ {\circ} + \Omega_ {\bar {J} ^ {'} X ^ {\circ}} \bar {J} ^ {'} X ^ {\circ} - l \{\theta (X ^ {\circ}) X ^ {\circ} + \theta (\bar {J} ^ {'} X ^ {\circ}) \bar {J} ^ {'} X ^ {\circ} \} \\ & \qquad - m \{\theta (X ^ {\circ}) f ^ {'} X ^ {\circ} + \theta (\bar {J} ^ {'} X ^ {\circ}) f ^ {' 2} X ^ {\circ} \}, \bar {J} ^ {'} W ^ {\circ} \Big) \\ & = g ^ {'} (\bar {J} ^ {'} X ^ {\circ}, \bar {A} _ {W ^ {\circ}} X ^ {\circ} + l \theta (W ^ {\circ}) X ^ {\circ} + m \theta (W ^ {\circ}) f ^ {'} X ^ {\circ}) \\ & + g ^ {'} (3 \bar {J} ^ {'} X ^ {\circ} + X ^ {\circ}, \bar {A} _ {W ^ {\circ}} \bar {J} ^ {'} X ^ {\circ} + l \theta (W ^ {\circ}) \bar {J} ^ {'} X ^ {\circ} + m \theta (W ^ {\circ}) f ^ {' 2} X ^ {\circ}), \end{array} \end{document} ]]></tex-math></disp-formula><p>for any <inline-formula><tex-math id="math-649"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle X ^ { \circ } \in \Gamma ( B _ { o } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-650"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula></p><p>Employing <xref ref-type="disp-formula" rid="equation-153">(52)</xref> on above equation, we attain</p><disp-formula id="equation-157"><tex-math id="math-651"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{l} 3 \{g ^ {'} (f ^ {'} X ^ {\circ}, \bar {A} _ {W ^ {\circ}} f ^ {'} X ^ {\circ}) + l \theta (W ^ {\circ}) g ^ {'} (X ^ {\circ}, f ^ {' 2} X ^ {\circ}) + m \theta (W ^ {\circ}) g ^ {'} (f ^ {'} X ^ {\circ}, f ^ {' 2} X ^ {\circ}) \} \\ = - 2 \{g ^ {'} (\bar {A} _ {W ^ {\circ}} f ^ {'} X ^ {\circ}, X ^ {\circ}) + l \theta (W ^ {\circ}) g ^ {'} (X ^ {\circ}, f ^ {'} X ^ {\circ}) + m \theta (W ^ {\circ}) g ^ {'} (X ^ {\circ}, f ^ {' 2} X ^ {\circ}) \}. \end{array} \end{document} ]]></tex-math></disp-formula><p><bold>Theorem 7.4.</bold><italic>A SG-lightlike submanifold </italic><inline-formula><tex-math id="math-652"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> ofa locally bronze semi-Riemannian manifold </italic><inline-formula><tex-math id="math-653"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { M } ^ { \circ } \end{document} ]]></tex-math></inline-formula><italic> with an </italic><inline-formula><tex-math id="math-654"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( l , m ) { - } t y p e \end{document} ]]></tex-math></inline-formula><italic> connection Ω</italic><sup><italic>¯</italic></sup><italic> is minimal if and only if</italic></p><disp-formula id="equation-158"><tex-math id="math-655"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}(i)\quad & \operatorname{trace}\bar{A}^{*}_{\xi_k}\big|_{S(TM^\circ)} = \operatorname{trace}\bar{A}_{W^\circ_\gamma}\big|_{S(TM^\circ)} = 0, \\(ii)\quad & \bar{g}'\big(\bar{D}^{\circ l}(X^\circ, W^\circ), Y^\circ\big) = l\theta(W^\circ)\bar{g}'(X^\circ, Y^\circ) + m\theta(W^\circ)\bar{g}'(f'X^\circ, Y^\circ),\end{align*} \end{document} ]]></tex-math></disp-formula><p><inline-formula><tex-math id="math-656"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \forall X ^ { \circ } , Y ^ { \circ } \in \Gamma ( R a d ( T M ^ { \circ } ) ) , W ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula> , where</p><p>dim <inline-formula><tex-math id="math-657"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( T M ^ { \circ } ) = m \end{document} ]]></tex-math></inline-formula> , dim <inline-formula><tex-math id="math-658"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle ( t r ( T M ^ { \circ } ) ) = n \end{document} ]]></tex-math></inline-formula> , dim <inline-formula><tex-math id="math-659"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \left( R a d ( T M ^ { \circ } ) \right) = r , \left\{ \xi _ { k } ^ { \circ } \right\} \end{document} ]]></tex-math></inline-formula> is a basis of <inline-formula><tex-math id="math-660"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle R a d ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-661"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle W _ { j } ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \perp } ) ) \end{document} ]]></tex-math></inline-formula> for <inline-formula><tex-math id="math-662"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle k \in \{ 1 , \ldots , r \} \end{document} ]]></tex-math></inline-formula> and <inline-formula><tex-math id="math-663"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle j \in \{ 1 , \dots , n - r \} \end{document} ]]></tex-math></inline-formula></p><p><italic>Proof</italic>. <inline-formula><tex-math id="math-664"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle M ^ { \circ } \end{document} ]]></tex-math></inline-formula> being minimal submanifold implies that</p><disp-formula id="equation-159"><tex-math id="math-665"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \left. \operatorname{trace} \bar {h} ^ {\circ} \right| _ {S (T M ^ {\circ})} = \left. \operatorname{trace} \bar {h} ^ {\circ} \right| _ {B _ {o}} + \left. \operatorname{trace} \bar {h} ^ {\circ} \right| _ {B ^ {\prime}} = \Sigma_ {i = 1} ^ {a} \bar {h} ^ {\circ} (B _ {i}, B _ {i}) + \Sigma_ {j = 1} ^ {b} \bar {h} ^ {\circ} (E _ {j}, E _ {j}) = 0, \end{document} ]]></tex-math></disp-formula><p>and <inline-formula><tex-math id="math-666"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { h ^ { \circ } } ^ { s } | _ { R a d ( T M ^ { \circ } ) } = 0 . \end{document} ]]></tex-math></inline-formula></p><p>If we choose an orthonormal basis of <inline-formula><tex-math id="math-667"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ } ) \end{document} ]]></tex-math></inline-formula> as <inline-formula><tex-math id="math-668"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ e _ { i } \} _ { i = 1 } ^ { m - r } \end{document} ]]></tex-math></inline-formula> , then we get</p><disp-formula id="equation-160"><tex-math id="math-669"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{align*}\operatorname{trace}\bar{h}^\circ\big|_{S(TM^\circ)} &= \sum_{i=1}^{a} \epsilon_i \left(\bar{h}^{\circ l}(e_i, e_i) + \bar{h}^{\circ s}(e_i, e_i)\right) + \sum_{j=1}^{b} \epsilon_j \left(\bar{h}^{\circ l}(e_j, e_j) + \bar{h}^{\circ s}(e_j, e_j)\right) \\&= \sum_{i=1}^{a} \epsilon_i \left[\frac{1}{r}\sum_{k=1}^{r} \bar{g}'\big(\bar{h}^{\circ l}(e_i, e_i), \xi_k^\circ\big) N_k^\circ \right. \\&\qquad \left. + \frac{1}{n-r}\sum_{j=1}^{n-r} \bar{g}'\big(\bar{h}^{\circ s}(e_i, e_i), W_j^\circ\big) W_j^\circ \right] \\&\quad + \sum_{j=1}^{b} \epsilon_j \left[\frac{1}{r}\sum_{k=1}^{r} \bar{g}'\big(\bar{h}^{\circ l}(e_j, e_j), \xi_k^\circ\big) N_k^\circ \right. \\&\qquad \left. + \frac{1}{n-r}\sum_{j=1}^{n-r} \bar{g}'\big(\bar{h}^{\circ s}(e_j, e_j), W_j^\circ\big) W_j^\circ \right],\end{align*} \end{document} ]]></tex-math></disp-formula><p>where <inline-formula><tex-math id="math-670"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \{ W _ { 1 } ^ { \circ } , W _ { 2 } ^ { \circ } , . . . . . , W _ { n - r } ^ { \circ } \} \end{document} ]]></tex-math></inline-formula> is an orthonormal basis of <inline-formula><tex-math id="math-671"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle S ( T M ^ { \circ \bot } ) \end{document} ]]></tex-math></inline-formula></p><p>Since, <inline-formula><tex-math id="math-672"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle { \bar { g } ^ { \prime } ( \bar { h ^ { \circ } } { } ^ { l } ( e _ { i } , e _ { i } ) , \xi _ { k } ^ { \circ } ) N _ { k } ^ { \circ } } \ = \ g ^ { \prime } ( \bar { A } _ { \xi _ { k } ^ { \circ } } ^ { * } e _ { i } , e _ { i } ) N _ { k } ^ { \circ } \ \mathrm { a n d } \ \bar { g } ^ { \prime } ( \bar { h ^ { \circ } } { } ^ { s } ( e _ { i } , e _ { i } ) , W _ { j } ^ { \circ } ) W _ { j } ^ { \circ } \ = \end{document} ]]></tex-math></inline-formula> k <inline-formula><tex-math id="math-673"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle g ^ { ' } ( \bar { A } _ { W _ { i } ^ { \circ } } e _ { i } , e _ { i } ) W _ { j } ^ { \circ } \end{document} ]]></tex-math></inline-formula> , we derive</p><p>traceh<sup>¯◦</sup>|S(TM◦) = traceA<sup>¯∗</sup>ξ◦k |Bo⊕B′ + traceA<sup>¯</sup>W◦j |Bo⊕B′ ,</p><p>Therefore, trace <inline-formula><tex-math id="math-674"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { A } _ { \xi _ { k } ^ { \circ } } ^ { * } | _ { B _ { o } \oplus B ^ { \prime } } \end{document} ]]></tex-math></inline-formula> and trace <inline-formula><tex-math id="math-675"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \bar { A } _ { W _ { i } ^ { \circ } } | _ { B _ { o } \oplus B ^ { \prime } } = 0 \end{document} ]]></tex-math></inline-formula></p><p>On the other hand, using concept of minimal SG-lightlike submanifold with equation <xref ref-type="disp-formula" rid="equation-50">(38)</xref>, we obtain</p><disp-formula id="equation-161"><tex-math id="math-676"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \begin{array}{r l} & {\bar {g} ^ {'} (\bar {h} ^ {\circ s} (X ^ {\circ}, Y ^ {\circ}), W ^ {\circ}) = - \bar {g} ^ {'} (\bar {D} ^ {\circ l} (X ^ {\circ}, W ^ {\circ}), Y ^ {\circ}) + l \theta (W ^ {\circ}) \bar {g} ^ {'} (X ^ {\circ}, Y ^ {\circ})} \\ & {\qquad + m \theta (W ^ {\circ}) \bar {g} ^ {'} (f ^ {'} X ^ {\circ}, Y ^ {\circ})} \end{array} \end{document} ]]></tex-math></disp-formula><p>∀ <inline-formula><tex-math id="math-677"><![CDATA[ \documentclass{article} \usepackage{amsmath} \begin{document} \displaystyle \ l ^ { \prime } X ^ { \circ } , Y ^ { \circ } \in \Gamma ( R a d ( T M ^ { \circ } ) ) , W ^ { \circ } \in \Gamma ( S ( T M ^ { \circ \bot } ) ) \end{document} ]]></tex-math></inline-formula> , which <italic>proof</italic> is completed. □</p></sec><sec id="sec-8"><title>8. CONCLUDING REMARKS</title><p>This research work has initiated the lightlike geometry of screen generic lightlike submanifolds in the bronze semi-Riemannian manifold equipped with an (l, m)- type connection.</p><p>The bronze Riemannian manifolds and bronze means are the impoprtant classes of metallic means family, are instrumental as the basis of proportion to design sculptures. These manifolds are of great use to physicists to analyze the behaviour of nonlinear dynamic systems in the transition from periodicity to semiperiodicity. The study undertaken suggests that there is a potential for further investigation of various metric or non-metric connections derived from (l, m)-type connection equipped with bronze semi-Riemannian manifold. Also, the geometry of screen generic lightlike submanifolds can be examined for various classes of metallic semi-Riemannian manifold equipped with distinct connections inherent to their structure. Also, the bronze semi-Riemannian manifolds, being intrinsically related to the theoretical explanation of behavior in quantum physics, can motivate the geometers to delve into the applications of this noteworthy area of study.</p></sec></body><back><sec sec-type="data-availability"><title>Data Availability Statement.</title><p>There were no data analyzed in this project.</p></sec><sec sec-type="author-contributions"><title>Author Contributions.</title><p>Conceptualization, R.K. and J.K.; methodology, J.K.; validation, R.K.; formal analysis, R.K. and J.K.; investigation, J.K.; resources, R.K. and J.K.; writing—original draft preparation, R.K.and J.K.; writing—review and editing, R.K., and J.K.; visualization, R.K.; supervision, J.K.; project administration, R.K. and J.K. 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