Exact solutions to complex Type IIB supergravity for complex superalgebra F (4) and its real forms

A bstract We construct the general local solutions to complexified Type IIB supergravity which are invariant under the complexified Lie superalgebra F (4). The geometry is a product of complexified maximally symmetric spaces $$ {\mathcal{M}}_{6\mathbb{C}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>M</mml:mi> <mml:mrow> <mml:mn>6</mml:mn> <mml:mi>ℂ</mml:mi> </mml:mrow> </mml:msub> </mml:math> and $$ {\mathcal{M}}_{2\mathbb{C}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>M</mml:mi> <mml:mrow> <mml:mn>2</mml:mn> <mml:mi>ℂ</mml:mi> </mml:mrow> </mml:msub> </mml:math> warped over a complexified surface Σ ℂ . We classify the reality conditions that may be imposed consistently to obtain real form solutions within real forms of complex Type IIB supergravity. The latter comprise standard Type IIB, Type IIB ⋆ and IIB ′ , as well as theories with 3, 5, 7 and 9 time-like directions. Our classification of real solutions is consistent with and exhausts the real forms of F (4), whose classification we confirm by elementary methods. The geometry of each real form solution is a product of real maximally symmetric spaces $$ {\mathcal{M}}_6 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>M</mml:mi> <mml:mn>6</mml:mn> </mml:msub> </mml:math> and $$ {\mathcal{M}}_2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>M</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:math> warped over a Riemann surface Σ, with various signatures. The real solutions include, among others, known AdS 6 × S 2 × Σ and AdS 2 × S 6 × Σ solutions to standard Type IIB as well as new solutions of the form dS 1,5 × S 2 × Σ in Type IIB ⋆ . There are no real forms of the complex solutions with $$ \mathbf{\mathfrak{so}}\left(7;\mathbb{R}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>so</mml:mi> <mml:mfenced> <mml:mn>7</mml:mn> <mml:mi>ℝ</mml:mi> </mml:mfenced> </mml:math> ⨁ $$ \mathbf{\mathfrak{so}}\left(3;\mathbb{R}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>so</mml:mi> <mml:mfenced> <mml:mn>3</mml:mn> <mml:mi>ℝ</mml:mi> </mml:mfenced> </mml:math> symmetry. We discuss the relevance of the complex solutions, and of analytic continuations from dS 1,5 × S 2 × Σ to S 6 × S 2 × Σ within complex Type IIB, in connection with holography for the polarized IKKT model.

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Journal
Journal of High Energy Physics
Published
2026-07-16
DOI
https://doi.org/10.1007/jhep07(2026)148
Primary Topic
Black Holes and Theoretical Physics
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article
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article

Exact solutions to complex Type IIB supergravity for complex superalgebra F (4) and its real forms

Christoph F. Uhlemann, Eric D’Hoker, Michael Gutperle
Journal of High Energy Physics
Black Holes and Theoretical Physics
article

Exact solutions to complex Type IIB supergravity for complex superalgebra F (4) and its real forms

Christoph F. Uhlemann, Eric D’Hoker, Michael Gutperle
article en

Abstract

A bstract We construct the general local solutions to complexified Type IIB supergravity which are invariant under the complexified Lie superalgebra F (4). The geometry is a product of complexified maximally symmetric spaces $$ {\mathcal{M}}_{6\mathbb{C}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>M</mml:mi> <mml:mrow> <mml:mn>6</mml:mn> <mml:mi>ℂ</mml:mi> </mml:mrow> </mml:msub> </mml:math> and $$ {\mathcal{M}}_{2\mathbb{C}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>M</mml:mi> <mml:mrow> <mml:mn>2</mml:mn> <mml:mi>ℂ</mml:mi> </mml:mrow> </mml:msub> </mml:math> warped over a complexified surface Σ ℂ . We classify the reality conditions that may be imposed consistently to obtain real form solutions within real forms of complex Type IIB supergravity. The latter comprise standard Type IIB, Type IIB ⋆ and IIB ′ , as well as theories with 3, 5, 7 and 9 time-like directions. Our classification of real solutions is consistent with and exhausts the real forms of F (4), whose classification we confirm by elementary methods. The geometry of each real form solution is a product of real maximally symmetric spaces $$ {\mathcal{M}}_6 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>M</mml:mi> <mml:mn>6</mml:mn> </mml:msub> </mml:math> and $$ {\mathcal{M}}_2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mi>M</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:math> warped over a Riemann surface Σ, with various signatures. The real solutions include, among others, known AdS 6 × S 2 × Σ and AdS 2 × S 6 × Σ solutions to standard Type IIB as well as new solutions of the form dS 1,5 × S 2 × Σ in Type IIB ⋆ . There are no real forms of the complex solutions with $$ \mathbf{\mathfrak{so}}\left(7;\mathbb{R}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>so</mml:mi> <mml:mfenced> <mml:mn>7</mml:mn> <mml:mi>ℝ</mml:mi> </mml:mfenced> </mml:math> ⨁ $$ \mathbf{\mathfrak{so}}\left(3;\mathbb{R}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>so</mml:mi> <mml:mfenced> <mml:mn>3</mml:mn> <mml:mi>ℝ</mml:mi> </mml:mfenced> </mml:math> symmetry. We discuss the relevance of the complex solutions, and of analytic continuations from dS 1,5 × S 2 × Σ to S 6 × S 2 × Σ within complex Type IIB, in connection with holography for the polarized IKKT model.

Journal of High Energy PhysicsVol. 2026(7)
Vrije Universiteit Brussel (BE), University of California System (US)
Openalex Percentile: Top 10%
Black Holes and Theoretical Physics
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