首页> 外文OA文献 >Anti-de Sitter Black Holes, Thermal Phase Transition and Holography in Higher Curvature Gravity
【2h】

Anti-de Sitter Black Holes, Thermal Phase Transition and Holography in Higher Curvature Gravity

机译:高曲率重力下的反de Sitter黑洞,热相变和全息术

代理获取
本网站仅为用户提供外文OA文献查询和代理获取服务,本网站没有原文。下单后我们将采用程序或人工为您竭诚获取高质量的原文,但由于OA文献来源多样且变更频繁,仍可能出现获取不到、文献不完整或与标题不符等情况,如果获取不到我们将提供退款服务。请知悉。

摘要

We study anti-de Sitter black holes and evaluate different thermodynamic quantities in the Einstein-Gauss-Bonnet and the general $R^2$ gravity theories. We examine the possibility of Hawking-Page type thermal phase transitions between AdS black hole and thermal anti-de Sitter space in such theories. In Einstein theory with a possible cosmological term, one observes a Hawking-Page phase transition only if the event horizon is a hypersurface of positive constant curvature ($k=1$). But in Einstein-Gauss-Bonnet gravity there can occur a similar transition even for a horizon of negative constant curvature ($k=-1$), which may allow one to study the boundary conformal theory with different background geometries. For the Gauss-Bonnet black holes, one can relate the entropy of the black hole as measured at horizon to a variation of the geometric property of the horizon based on first law and Noether charge. With $({Riemann})^2$ terms, however, we can do this only approximately, and the two results agree in the limit $r_H>>L$, the size of the horizon is much bigger than the AdS curvature. In $({Riemann})^2$ gravity, we establish certain relations between bulk data associated with the AdS black hole in five dimensions and boundary data defined on the horizon of the AdS geometry, in which case we do not expect a sensible holographic dual. We also give a heuristic approach to estimate the difference between Hubble entropy and Bakenstein-Hawking entropy with $({Riemann})^2$ term.
机译:我们研究了反de Sitter黑洞,并在Einstein-Gauss-Bonnet和一般的$ R ^ 2 $重力理论中评估了不同的热力学量。在此类理论中,我们研究了AdS黑洞与热反de Sitter空间之间的Hawking-Page型热相变的可能性。在具有可能的宇宙学术语的爱因斯坦理论中,只有当事件层是正曲率恒定的超曲面($ k = 1 $)时,才观察到霍金-佩奇相变。但是在爱因斯坦-高斯-邦尼特引力中,即使对于负恒定曲率的地平线($ k = -1 $),也会发生类似的过渡,这可能使人们可以研究具有不同背景几何形状的边界共形理论。对于Gauss-Bonnet黑洞,可以根据第一定律和Noether电荷将在视界测得的黑洞的熵与视界的几何特性变化联系起来。但是,在$({Riemann})^ 2 $项的情况下,我们只能近似执行此操作,并且两个结果在限制$ r_H >> L $中一致,地平线的大小远大于AdS曲率。在$({Riemann})^ 2 $的重力下,我们在五个维度上与AdS黑洞关联的整体数据与在AdS几何图形的地平线上定义的边界数据之间建立了一定的关系,在这种情况下,我们不希望出现明显的全息图双。我们还给出了一种启发式方法,以$({Riemann})^ 2 $项估计Hubble熵和Bakenstein-Hawking熵之间的差异。

著录项

  • 作者

    Cho, Y M; Neupane, I P;

  • 作者单位
  • 年度 2002
  • 总页数
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类

相似文献

  • 外文文献
  • 中文文献
  • 专利
代理获取

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号