Supersymmetric $$AdS_6$$ A d S 6 black holes from ISO(3) $$\times $$ × U(1) F(4) gauged supergravity
Abstract We study supersymmetric $$AdS_6$$ A d S 6 black holes from matter-coupled F(4) gauged supergravity coupled to four vector multiplets with $$ISO(3)\times U(1)$$ I S O ( 3 ) × U ( 1 ) gauge group. This gauged supergravity admits a maximally supersymmetric $$AdS_6$$ A d S 6 vacuum with $$SO(3)...
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2025-02-01
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| Series: | European Physical Journal C: Particles and Fields |
| Online Access: | https://doi.org/10.1140/epjc/s10052-025-13880-0 |
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| author | Parinya Karndumri |
| author_facet | Parinya Karndumri |
| author_sort | Parinya Karndumri |
| collection | DOAJ |
| description | Abstract We study supersymmetric $$AdS_6$$ A d S 6 black holes from matter-coupled F(4) gauged supergravity coupled to four vector multiplets with $$ISO(3)\times U(1)$$ I S O ( 3 ) × U ( 1 ) gauge group. This gauged supergravity admits a maximally supersymmetric $$AdS_6$$ A d S 6 vacuum with $$SO(3)\subset ISO(3)$$ S O ( 3 ) ⊂ I S O ( 3 ) symmetry. We find a number of new supersymmetric $$AdS_2\times \mathcal {M}_4$$ A d S 2 × M 4 solutions by performing topological twists along $$\mathcal {M}_4$$ M 4 . For $$\mathcal {M}_4$$ M 4 being a product of two Riemann surfaces $$\Sigma \times \widetilde{\Sigma }$$ Σ × Σ ~ , we perform a twist by $$SO(2)\times U(1)$$ S O ( 2 ) × U ( 1 ) gauge fields and find $$AdS_2\times \Sigma \times \widetilde{\Sigma }$$ A d S 2 × Σ × Σ ~ solutions for at least one of the Riemann surface being negatively curved. For $$\mathcal {M}_4$$ M 4 being a Kahler four-cycle $$\mathcal {M}_{\text {K}4}$$ M K 4 , a twist by $$SO(2)\times U(1)$$ S O ( 2 ) × U ( 1 ) gauge fields leads to $$AdS_2\times \mathcal {M}_{\text {K}4}^-$$ A d S 2 × M K 4 - solutions for negatively curved $$\mathcal {M}_{\text {K}4}$$ M K 4 . Finally, performing a twist by turning on SO(3) gauge fields in the case of $$\mathcal {M}_4$$ M 4 being a Cayley four-cycle $$\mathcal {M}_{\text {C}4}$$ M C 4 also leads to $$AdS_2\times \mathcal {M}_{\text {C}4}^-$$ A d S 2 × M C 4 - solutions for negatively curved $$\mathcal {M}_{\text {C}4}$$ M C 4 . We give numerical black hole solutions interpolating between all of these $$AdS_2\times \mathcal {M}_4$$ A d S 2 × M 4 near horizon geometries and the asymptotically locally $$AdS_6$$ A d S 6 vacuum. It is also possible to uplift all of these solutions to type IIB theory via consistent truncations on $$S^2\times \Sigma $$ S 2 × Σ leading to a new class of supersymmetric $$AdS_2\times \mathcal {M}_4\times S^2\times \Sigma $$ A d S 2 × M 4 × S 2 × Σ solutions. |
| format | Article |
| id | doaj-art-8fbb6a876bf24ffa8634b4a78273ad1c |
| institution | Kabale University |
| issn | 1434-6052 |
| language | English |
| publishDate | 2025-02-01 |
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| series | European Physical Journal C: Particles and Fields |
| spelling | doaj-art-8fbb6a876bf24ffa8634b4a78273ad1c2025-02-09T12:51:33ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60522025-02-0185211510.1140/epjc/s10052-025-13880-0Supersymmetric $$AdS_6$$ A d S 6 black holes from ISO(3) $$\times $$ × U(1) F(4) gauged supergravityParinya Karndumri0String Theory and Supergravity Group, Department of Physics, Faculty of Science, Chulalongkorn UniversityAbstract We study supersymmetric $$AdS_6$$ A d S 6 black holes from matter-coupled F(4) gauged supergravity coupled to four vector multiplets with $$ISO(3)\times U(1)$$ I S O ( 3 ) × U ( 1 ) gauge group. This gauged supergravity admits a maximally supersymmetric $$AdS_6$$ A d S 6 vacuum with $$SO(3)\subset ISO(3)$$ S O ( 3 ) ⊂ I S O ( 3 ) symmetry. We find a number of new supersymmetric $$AdS_2\times \mathcal {M}_4$$ A d S 2 × M 4 solutions by performing topological twists along $$\mathcal {M}_4$$ M 4 . For $$\mathcal {M}_4$$ M 4 being a product of two Riemann surfaces $$\Sigma \times \widetilde{\Sigma }$$ Σ × Σ ~ , we perform a twist by $$SO(2)\times U(1)$$ S O ( 2 ) × U ( 1 ) gauge fields and find $$AdS_2\times \Sigma \times \widetilde{\Sigma }$$ A d S 2 × Σ × Σ ~ solutions for at least one of the Riemann surface being negatively curved. For $$\mathcal {M}_4$$ M 4 being a Kahler four-cycle $$\mathcal {M}_{\text {K}4}$$ M K 4 , a twist by $$SO(2)\times U(1)$$ S O ( 2 ) × U ( 1 ) gauge fields leads to $$AdS_2\times \mathcal {M}_{\text {K}4}^-$$ A d S 2 × M K 4 - solutions for negatively curved $$\mathcal {M}_{\text {K}4}$$ M K 4 . Finally, performing a twist by turning on SO(3) gauge fields in the case of $$\mathcal {M}_4$$ M 4 being a Cayley four-cycle $$\mathcal {M}_{\text {C}4}$$ M C 4 also leads to $$AdS_2\times \mathcal {M}_{\text {C}4}^-$$ A d S 2 × M C 4 - solutions for negatively curved $$\mathcal {M}_{\text {C}4}$$ M C 4 . We give numerical black hole solutions interpolating between all of these $$AdS_2\times \mathcal {M}_4$$ A d S 2 × M 4 near horizon geometries and the asymptotically locally $$AdS_6$$ A d S 6 vacuum. It is also possible to uplift all of these solutions to type IIB theory via consistent truncations on $$S^2\times \Sigma $$ S 2 × Σ leading to a new class of supersymmetric $$AdS_2\times \mathcal {M}_4\times S^2\times \Sigma $$ A d S 2 × M 4 × S 2 × Σ solutions.https://doi.org/10.1140/epjc/s10052-025-13880-0 |
| spellingShingle | Parinya Karndumri Supersymmetric $$AdS_6$$ A d S 6 black holes from ISO(3) $$\times $$ × U(1) F(4) gauged supergravity European Physical Journal C: Particles and Fields |
| title | Supersymmetric $$AdS_6$$ A d S 6 black holes from ISO(3) $$\times $$ × U(1) F(4) gauged supergravity |
| title_full | Supersymmetric $$AdS_6$$ A d S 6 black holes from ISO(3) $$\times $$ × U(1) F(4) gauged supergravity |
| title_fullStr | Supersymmetric $$AdS_6$$ A d S 6 black holes from ISO(3) $$\times $$ × U(1) F(4) gauged supergravity |
| title_full_unstemmed | Supersymmetric $$AdS_6$$ A d S 6 black holes from ISO(3) $$\times $$ × U(1) F(4) gauged supergravity |
| title_short | Supersymmetric $$AdS_6$$ A d S 6 black holes from ISO(3) $$\times $$ × U(1) F(4) gauged supergravity |
| title_sort | supersymmetric ads 6 a d s 6 black holes from iso 3 times u 1 f 4 gauged supergravity |
| url | https://doi.org/10.1140/epjc/s10052-025-13880-0 |
| work_keys_str_mv | AT parinyakarndumri supersymmetricads6ads6blackholesfromiso3timesu1f4gaugedsupergravity |