From minimal strings towards Jackiw-Teitelboim gravity: On their resurgence, resonance, and black holes

P. Gregori, R. Schiappa
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Abstract

Two remarkable facts about Jackiw-Teitelboim two-dimensional dilaton-gravity have been recently uncovered: this theory is dual to an ensemble of quantum mechanical theories; and such ensembles are described by a random matrix model which itself may be regarded as a special (large matter-central-charge) limit of minimal string theory. This work addresses this limit, putting it in its broader matrix-model context; comparing results between multicritical models and minimal strings (i.e., changing in-between multicritical and conformal backgrounds); and in both cases making the limit of large matter-central-charge precise (as such limit can also be defined for the multicritical series). These analyses are first done via spectral geometry, at both perturbative and nonperturbative levels, addressing the resurgent large-order growth of perturbation theory, alongside a calculation of nonperturbative instanton-actions and corresponding Stokes data. This calculation requires an algorithm to reach large-order, which is valid for arbitrary two-dimensional topological gravity. String equations---as derived from the Gel'fand-Dikii construction of the resolvent---are analyzed in both multicritical and minimal string theoretic contexts, and studied both perturbatively and nonperturbatively (always matching against the earlier spectral-geometry computations). The resulting solutions, as described by resurgent transseries, are shown to be resonant. The large matter-central-charge limit is addressed---in the string-equation context---and, in particular, the string equation for Jackiw-Teitelboim gravity is obtained to next derivative-orders, beyond the known genus-zero case (its possible exact-form is also discussed). Finally, a discussion of gravitational perturbations to Schwarzschild-like black hole solutions in these minimal-string models, regarded as deformations of Jackiw-Teitelboim gravity, is included---alongside a brief discussion of quasinormal modes.
从最小弦到杰克维-特尔布依姆引力:关于它们的复活、共振和黑洞
最近发现了关于杰克维-泰特博伊姆二维稀拉顿引力的两个非凡事实:这一理论与量子力学理论的集合是对偶的;这种集合由随机矩阵模型描述,而随机矩阵模型本身可被视为极小弦理论的一个特殊(大物质-中心电荷)极限。这项工作涉及这一极限,将其置于更广泛的矩阵模型背景中;比较多临界模型和极小弦之间的结果(即在多临界背景和保角背景之间变化);并在两种情况下都使大物质-中心电荷极限精确化(因为这种极限也可以为多临界序列定义)。这些分析首先是通过谱几何在微扰和非微扰层面上完成的,解决了微扰理论的大阶增长问题,同时还计算了非微扰瞬子作用和相应的斯托克斯数据。这种计算需要一种达到大阶的算法,它适用于任意二维拓扑引力。在多临界和最小弦理论的背景下分析了弦方程--从Gel'fand-Dikii的解析构造中导出--并研究了扰动和非扰动(始终与先前的谱几何计算相匹配)。结果表明,所得到的解决方案,正如回升跨序列所描述的那样,是共振的。在弦方程的背景下,讨论了大物质-中心-电荷极限,特别是在已知的零属情况之外,获得了杰克维-泰特博伊姆引力的弦方程的下一个导数阶(还讨论了其可能的精确形式)。最后,我们还讨论了这些最小弦模型中类似于施瓦兹丘尔德黑洞解的引力扰动,将其视为杰克维-泰特博伊姆引力的变形--同时简要讨论了准正常模式。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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