<p>We construct new families of supersymmetric <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1916_Article_IEq1.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="76" /> </InlineMediaObject> <EquationSource Format="TEX">\({\textrm{AdS}}_2\times \mathbb {M}_4\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>AdS</mtext> <mn>2</mn> </msub> <mo>×</mo> <msub> <mi mathvariant="double-struck">M</mi> <mn>4</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> solutions of <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1916_Article_IEq2.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(D=6\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>D</mi> <mo>=</mo> <mn>6</mn> </mrow> </math></EquationSource> </InlineEquation> gauged supergravity and <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1916_Article_IEq3.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="76" /> </InlineMediaObject> <EquationSource Format="TEX">\({\textrm{AdS}}_3\times \mathbb {M}_4\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mtext>AdS</mtext> <mn>3</mn> </msub> <mo>×</mo> <msub> <mi mathvariant="double-struck">M</mi> <mn>4</mn> </msub> </mrow> </math></EquationSource> </InlineEquation> solutions of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1916_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(D=7\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>D</mi> <mo>=</mo> <mn>7</mn> </mrow> </math></EquationSource> </InlineEquation> gauged supergravity, where <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1916_Article_IEq5.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {M}_4\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">M</mi> <mn>4</mn> </msub> </math></EquationSource> </InlineEquation> are four-dimensional toric orbifolds with four fixed points. These are presented in a unified fashion that highlights their common underlying geometry. The <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1916_Article_IEq6.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(D=6\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>D</mi> <mo>=</mo> <mn>6</mn> </mrow> </math></EquationSource> </InlineEquation> solutions uplift to massive type IIA and describe the near-horizon limit of D4-branes wrapped on <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1916_Article_IEq7.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {M}_4\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">M</mi> <mn>4</mn> </msub> </math></EquationSource> </InlineEquation>, while the <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1916_Article_IEq8.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="46" /> </InlineMediaObject> <EquationSource Format="TEX">\(D=7\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>D</mi> <mo>=</mo> <mn>7</mn> </mrow> </math></EquationSource> </InlineEquation> solutions uplift to <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1916_Article_IEq9.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="54" /> </InlineMediaObject> <EquationSource Format="TEX">\(D=11\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>D</mi> <mo>=</mo> <mn>11</mn> </mrow> </math></EquationSource> </InlineEquation> supergravity and describe the near-horizon limit of M5-branes wrapped on <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11005_2025_1916_Article_IEq10.gif" Format="GIF" Height="16" Rendition="HTML" Resolution="72" Type="Linedraw" Width="19" /> </InlineMediaObject> <EquationSource Format="TEX">\(\mathbb {M}_4\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="double-struck">M</mi> <mn>4</mn> </msub> </math></EquationSource> </InlineEquation>. We reproduce the entropy and gravitational central charge of the two families by extremizing a function constructed gluing the orbifold gravitational blocks proposed in Faedo et al. (Lett Math Phys 113:51, 2023. <a href="https://doi.org/10.1007/s11005-023-01671-1">https://doi.org/10.1007/s11005-023-01671-1</a>. <a href="http://arxiv.org/abs/2210.16128">arXiv:2210.16128</a>).</p>

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Branes wrapped on quadrilaterals

  • Federico Faedo,
  • Alessio Fontanarossa,
  • Dario Martelli

摘要

We construct new families of supersymmetric \({\textrm{AdS}}_2\times \mathbb {M}_4\) AdS 2 × M 4 solutions of \(D=6\) D = 6 gauged supergravity and \({\textrm{AdS}}_3\times \mathbb {M}_4\) AdS 3 × M 4 solutions of \(D=7\) D = 7 gauged supergravity, where \(\mathbb {M}_4\) M 4 are four-dimensional toric orbifolds with four fixed points. These are presented in a unified fashion that highlights their common underlying geometry. The \(D=6\) D = 6 solutions uplift to massive type IIA and describe the near-horizon limit of D4-branes wrapped on \(\mathbb {M}_4\) M 4 , while the \(D=7\) D = 7 solutions uplift to \(D=11\) D = 11 supergravity and describe the near-horizon limit of M5-branes wrapped on \(\mathbb {M}_4\) M 4 . We reproduce the entropy and gravitational central charge of the two families by extremizing a function constructed gluing the orbifold gravitational blocks proposed in Faedo et al. (Lett Math Phys 113:51, 2023. https://doi.org/10.1007/s11005-023-01671-1. arXiv:2210.16128).