<p>We classify Riemannian <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\text {spin}^c\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>spin</mtext> <mi>c</mi> </msup> </math></EquationSource> </InlineEquation> manifolds carrying a type I imaginary generalized Killing spinor, by explicitly constructing a parallel spinor on each leaf of the canonical foliation given by the Dirac current. We also provide a class of Riemannian <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\text {spin}^c\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>spin</mtext> <mi>c</mi> </msup> </math></EquationSource> </InlineEquation> manifolds carrying a type II imaginary generalized Killing spinor, by considering spacelike hypersurfaces of Lorentzian <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\text {spin}^c\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>spin</mtext> <mi>c</mi> </msup> </math></EquationSource> </InlineEquation> manifolds. We carry out much of the work in the setting of semi-Riemannian <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\text {spin}^c\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>spin</mtext> <mi>c</mi> </msup> </math></EquationSource> </InlineEquation>-manifolds carrying generalized Killing spinors, allowing us to draw conclusions in this setting as well. In this context, the Dirac current is not always a closed vector field. We circumvent this in even dimensions, by considering a modified Dirac current, which is closed in the cases when the original Dirac current is not. On the path to these results, we also study semi-Riemannian manifolds carrying closed and conformal vector fields.</p>

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Semi-Riemannian \(\text {spin}^c\) manifolds carrying generalized Killing spinors and the classification of Riemannian \(\text {spin}^c\) manifolds admitting a type I imaginary generalized Killing spinor

  • Samuel Lockman

摘要

We classify Riemannian \(\text {spin}^c\) spin c manifolds carrying a type I imaginary generalized Killing spinor, by explicitly constructing a parallel spinor on each leaf of the canonical foliation given by the Dirac current. We also provide a class of Riemannian \(\text {spin}^c\) spin c manifolds carrying a type II imaginary generalized Killing spinor, by considering spacelike hypersurfaces of Lorentzian \(\text {spin}^c\) spin c manifolds. We carry out much of the work in the setting of semi-Riemannian \(\text {spin}^c\) spin c -manifolds carrying generalized Killing spinors, allowing us to draw conclusions in this setting as well. In this context, the Dirac current is not always a closed vector field. We circumvent this in even dimensions, by considering a modified Dirac current, which is closed in the cases when the original Dirac current is not. On the path to these results, we also study semi-Riemannian manifolds carrying closed and conformal vector fields.