<p>This study investigates the geometric properties of almost <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\varvec{\eta }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">η</mi> </mrow> </math></EquationSource> </InlineEquation>-Ricci-Bourguignon solitons on para-Kenmotsu manifolds. First, it is shown that if the metric <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\varvec{g}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">g</mi> </mrow> </math></EquationSource> </InlineEquation> on a para-Kenmotsu manifold admits an almost <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\varvec{\eta }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">η</mi> </mrow> </math></EquationSource> </InlineEquation>-Ricci-Bourguignon soliton and the Reeb vector field <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\varvec{\xi }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">ξ</mi> </mrow> </math></EquationSource> </InlineEquation> preserves the function <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\varvec{\mu }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">μ</mi> </mrow> </math></EquationSource> </InlineEquation>, then the manifold <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\varvec{M}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">M</mi> </mrow> </math></EquationSource> </InlineEquation> is Einstein. Next, we establish that if <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\varvec{g}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">g</mi> </mrow> </math></EquationSource> </InlineEquation> is an almost <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\varvec{\eta }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">η</mi> </mrow> </math></EquationSource> </InlineEquation>-Ricci-Bourguignon soliton and the vector field <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\varvec{\xi }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">ξ</mi> </mrow> </math></EquationSource> </InlineEquation> leaves both <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\varvec{\lambda + \rho r}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">λ</mi> <mo mathvariant="bold">+</mo> <mi mathvariant="bold-italic">ρ</mi> <mi mathvariant="bold-italic">r</mi> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\varvec{\mu }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">μ</mi> </mrow> </math></EquationSource> </InlineEquation> invariant, then the soliton reduces to an <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\varvec{\eta }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">η</mi> </mrow> </math></EquationSource> </InlineEquation>-Ricci-Bourguignon soliton. Finally, we prove that if <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\varvec{g}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">g</mi> </mrow> </math></EquationSource> </InlineEquation> is a gradient almost <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\varvec{\eta }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">η</mi> </mrow> </math></EquationSource> </InlineEquation>-Ricci-Bourguignon soliton, then <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\varvec{M}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="bold-italic">M</mi> </mrow> </math></EquationSource> </InlineEquation> is necessarily Einstein.</p>

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GEOMETRIC CHARACTERIZATIONS OF ALMOST \(\eta \)-RICCI-BOURGUIGNON SOLITONS ON PARA-KENMOTSU MANIFOLDS

  • H. G. Nagaraja,
  • Pavithra R. C.

摘要

This study investigates the geometric properties of almost \(\varvec{\eta }\) η -Ricci-Bourguignon solitons on para-Kenmotsu manifolds. First, it is shown that if the metric \(\varvec{g}\) g on a para-Kenmotsu manifold admits an almost \(\varvec{\eta }\) η -Ricci-Bourguignon soliton and the Reeb vector field \(\varvec{\xi }\) ξ preserves the function \(\varvec{\mu }\) μ , then the manifold \(\varvec{M}\) M is Einstein. Next, we establish that if \(\varvec{g}\) g is an almost \(\varvec{\eta }\) η -Ricci-Bourguignon soliton and the vector field \(\varvec{\xi }\) ξ leaves both \(\varvec{\lambda + \rho r}\) λ + ρ r and \(\varvec{\mu }\) μ invariant, then the soliton reduces to an \(\varvec{\eta }\) η -Ricci-Bourguignon soliton. Finally, we prove that if \(\varvec{g}\) g is a gradient almost \(\varvec{\eta }\) η -Ricci-Bourguignon soliton, then \(\varvec{M}\) M is necessarily Einstein.