Rotating black holes in the FI-gauged N = 2, D = 4 ℂ P ¯ n $$ \overline{\mathbb{C}\mathrm{P}}}^{\mathrm{n}} $$ model

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: Rotating black holes in the FI-gauged N = 2, D = 4 ℂ P ¯ n $$ \overline{\mathbb{C}\mathrm{P}}}^{\mathrm{n}} $$ model ; volume:2019 ; number:3 ; day:25 ; month:3 ; year:2019 ; pages:1-30 ; date:3.2019
Journal of high energy physics ; 2019, Heft 3 (25.3.2019), 1-30, 3.2019

Creator: Daniele, Nicoletta
Faedo, Federico
Klemm, Dietmar
Ramírez, Pedro F.

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP03(2019)151

URN: urn:nbn:de:101:1-2019041722075009598155

Rights: Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 14.08.2025, 10:44 AM CEST

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Daniele, Nicoletta
Faedo, Federico
Klemm, Dietmar
Ramírez, Pedro F.
SpringerLink (Online service)

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Rotating black holes in the FI-gauged N = 2, D = 4 ℂ P ¯ n $$ \overline{\mathbb{C}\mathrm{P}}}^{\mathrm{n}} $$ model

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Other Objects (12)

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T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and LST

T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed nonlinear Schrödinger

Charmonium-like resonances with JPC = 0++, 2++ in coupled D D ¯ $$ \mathrmD}\overline{\mathrm{D}} $$ , D s D ¯ s $$ \mathrm{D}}_{\mathrm{s}}{\overline{\mathrm{D}}}_{\mathrm{s}} $$ scattering on the lattice

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Probing the top-quark width through ratios of resonance contributions of e + e − → W + W − b b ¯ $$ \mathrm{e}}^{+}{\mathrm{e}}^{-}\to \mathrm{W}}^{+}{\mathrm{W}}^{-}\mathrm{b}\overline{\mathrm{b}} $$

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T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed 2D quantum field theories

TsT, T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ and black strings

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The T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ perturbation and its geometric interpretation

Entanglement renormalization of a T T ¯ $$ \mathrmT}\overline{\mathrm{T}} $$ -deformed CFT

Supersymmetric Casimir energy and S L 3 ℤ $$ \mathrmS}\mathrm{L}\left(3,\mathrm{\mathbb{Z}}\right) $$ transformations

SL 2 ℝ × U 1 U 1 $$ \frac\mathrm{SL}\left(2,\mathrm{\mathbb{R}}\right)\times \mathrmU}(1)}{\mathrm{U}(1)} $$ CFT, NS5+F1 system and single trace T T ¯ $$ T\overlineT} $$

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