从热力学角度看引力的标量张量理论

Krishnakanta Bhattacharya, Sumanta Chakraborty
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摘要

在广义相对论和兰克佐斯-洛夫洛克引力理论中,人们发现,时空中任何主体区域的诺特电荷密度都可以解释为边界表面的热含量。此外,研究还发现,时空的动力学演化可以解释为脱离了正确定义的体自由度和表自由度之间的 "等分"。我们发现,同样的解释也适用于标量张量引力理论,在这种情况下,引力不仅受标量张量的介导,也受标量场的介导。此外,这些结果在与标量张量理论相关的两个框架(即乔丹框架和爱因斯坦框架)中都成立。然而,事实证明,在乔丹框架中,标量张量理论有两种动力学上等价的表示,它们的区别在于作用中的总导数,而这两种表示在热力学上是等价的。因此,热力学对标量张量理论的各种表示都很敏感。这不仅意味着引力的热力学描述具有超越广义相对论的稳健性,而且通过区分各种动力学等价表征,说明了热力学描述的重要性。
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Scalar-tensor theories of gravity from a thermodynamic viewpoint
In both general relativity and Lanczos-Lovelock theories of gravity, it has been found that the Noether charge density in any bulk region of spacetime can be interpreted as the heat content of the boundary surface. In addition, it was found that the dynamical evolution of spacetime can be interpreted as the departure from an ``equipartition" between properly defined bulk and surface degrees of freedom. We find that the same interpretations are valid for scalar-tensor theories of gravity, in which case the gravity is mediated by the metric tensor as well as by the scalar field. Moreover, these results hold in both the frames associated with the scalar-tensor theory, namely the Jordan and the Einstein frames. However, it turns out that there are two dynamically equivalent representations of the scalar-tensor theory in the Jordan frame, differing by total derivatives in the action, which are thermodynamically inequivalent. Thus thermodynamics is sensitive to various representations of scalar-tensor theories. This not only implies the robustness of the thermodynamic description of gravity beyond general relativity, but also depicts the importance of having a thermodynamic description by distinguishing various dynamically equivalent representations.
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