{
  "_oai": {
    "updated": "2022-12-30T00:30:26Z", 
    "id": "oai:repo.scoap3.org:74809", 
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  "authors": [
    {
      "raw_name": "Ger\u00f3nimo Caselli", 
      "affiliations": [
        {
          "country": "Argentina", 
          "value": "Departamento de F\u00edsica, Universidad Nacional de Rosario, Av. Pellegrini 250, Rosario, Santa Fe, Argentina"
        }
      ], 
      "surname": "Caselli", 
      "given_names": "Ger\u00f3nimo", 
      "full_name": "Caselli, Ger\u00f3nimo"
    }, 
    {
      "raw_name": "Gaston Giribet", 
      "affiliations": [
        {
          "country": "USA", 
          "value": "Department of Physics, New York University. 726 Broadway, New York, New York 10003, USA"
        }
      ], 
      "surname": "Giribet", 
      "given_names": "Gaston", 
      "full_name": "Giribet, Gaston"
    }, 
    {
      "raw_name": "Andr\u00e9s Goya", 
      "affiliations": [
        {
          "country": "Argentina", 
          "value": "Instituto de Astronom\u00eda y F\u00edsica del Espacio, Ciudad Universitaria, Casilla de Correo 67, Sucursal 28, 1428, Buenos Aires, Argentina"
        }
      ], 
      "surname": "Goya", 
      "given_names": "Andr\u00e9s", 
      "full_name": "Goya, Andr\u00e9s"
    }
  ], 
  "titles": [
    {
      "source": "APS", 
      "title": "Critical points of warped <math><mrow><mi>AdS</mi><mo>/</mo><mi>CFT</mi></mrow></math> and higher-curvature gravity"
    }
  ], 
  "dois": [
    {
      "value": "10.1103/PhysRevD.106.126026"
    }
  ], 
  "publication_info": [
    {
      "journal_volume": "106", 
      "journal_title": "Physical Review D", 
      "material": "article", 
      "journal_issue": "12", 
      "year": 2022
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2022-12-30T00:30:20.899116", 
    "source": "APS", 
    "method": "APS", 
    "submission_number": "183a9b6287d911ed93fbd61508239648"
  }, 
  "page_nr": [
    11
  ], 
  "license": [
    {
      "url": "https://creativecommons.org/licenses/by/4.0/", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "statement": "Published by the American Physical Society", 
      "year": "2022"
    }
  ], 
  "control_number": "74809", 
  "record_creation_date": "2022-12-29T16:30:05.961483", 
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  "collections": [
    {
      "primary": "HEP"
    }, 
    {
      "primary": "Citeable"
    }, 
    {
      "primary": "Published"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-th"
      ], 
      "value": "2209.01287"
    }
  ], 
  "abstracts": [
    {
      "source": "APS", 
      "value": "Warped anti-de Sitter (WAdS)/warped conformal field theory (WCFT) correspondence is an interesting realization of non-AdS holography. It relates three-dimensional warped anti-de Sitter (<math><mrow><msub><mrow><mi>WAdS</mi></mrow><mrow><mn>3</mn></mrow></msub></mrow></math>) spaces to a special class of two-dimensional quantum field theory with chiral scaling symmetry that acts only on right-moving modes. The latter are often called warped conformal field theories (<math><mrow><msub><mrow><mi>WCFT</mi></mrow><mrow><mn>2</mn></mrow></msub></mrow></math>), and their existence makes WAdS/WCFT particularly interesting as a tool to investigate a new type of two-dimensional conformal structure. Besides, WAdS/WCFT is interesting because it enables one to apply holographic techniques to the microstate counting problem of non-AdS, nonsupersymmetric black holes. Asymptotically <math><mrow><msub><mrow><mi>WAdS</mi></mrow><mrow><mn>3</mn></mrow></msub></mrow></math> black holes (<math><mrow><msub><mrow><mi>WBH</mi></mrow><mrow><mn>3</mn></mrow></msub></mrow></math>) appear as solutions of topologically massive theories, Chern-Simons theories, and many other models. Here, we explore <math><msub><mrow><mi>WBH</mi></mrow><mn>3</mn></msub><mo>\u00d7</mo><msub><mi>\u03a3</mi><mrow><mi>D</mi><mo>\u2212</mo><mn>3</mn></mrow></msub></math> solutions of <math><mi>D</mi></math>-dimensional higher-curvature gravity, with <math><msub><mi>\u03a3</mi><mrow><mi>D</mi><mo>\u2212</mo><mn>3</mn></mrow></msub></math> being different internal manifolds, typically given by products of deformations of hyperbolic spaces, although we also consider warped products with time-dependent deformations. These geometries are solutions of the second order higher-curvature theory at special (critical) points of the parameter space, where the theory exhibits a sort of degeneracy. We argue that the dual (W)CFT at those points is actually trivial. In many respects, these critical points of <math><msub><mtext>WAdS</mtext><mn>3</mn></msub><mo>\u00d7</mo><msub><mi>\u03a3</mi><mrow><mi>D</mi><mo>\u2212</mo><mn>3</mn></mrow></msub></math> vacua are the squashed/stretched analogs of the <math><mrow><msub><mrow><mi>AdS</mi></mrow><mrow><mi>D</mi></mrow></msub></mrow></math> Chern-Simons point of Lovelock gravity."
    }
  ], 
  "imprints": [
    {
      "date": "2022-12-29", 
      "publisher": "APS"
    }
  ]
}