Partition functions for non-commutative harmonic oscillators and related divergent series

Kazufumi Kimoto, Masato Wakayama
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Abstract

In the standard normalization, the eigenvalues of the quantum harmonic oscillator are given by positive half-integers with the Hermite functions as eigenfunctions. Thus, its spectral zeta function is essentially given by the Riemann zeta function. The heat kernel (or propagator) of the quantum harmonic oscillator (qHO) is given by the Mehler formula, and the partition function is obtained by taking its trace. In general, the spectral zeta function of the given system is obtained by the Mellin transform of its partition function. In the case of non-commutative harmonic oscillators (NCHO), however, the heat kernel and partition functions are still unknown, although meromorphic continuation of the corresponding spectral zeta function and special values at positive integer points have been studied. On the other hand, explicit formulas for the heat kernel and partition function have been obtained for the quantum Rabi model (QRM), which is the simplest and most fundamental model for light and matter interaction in addition to having the NCHO as a covering model. In this paper, we propose a notion of the for a quantum interaction model if the corresponding spectral zeta function can be meromorphically continued to the whole complex plane. The quasi-partition function for qHO and QRM actually gives the partition function. Assuming that this holds for the NCHO (currently a conjecture), we can find various interesting properties for the spectrum of the NCHO. Moreover, although we cannot expect any functional equation of the spectral zeta function for the quantum interaction models, we try to seek if there is some relation between the special values at positive and negative points. Attempting to seek this, we encounter certain divergent series expressing formally the Hurwitz zeta function by calculating integrals of the partition functions. We then give two interpretations of these divergent series by the Borel summation and -adically convergent series defined by the -adic Hurwitz zeta function.
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非交换调和振荡器的分割函数及相关发散级数
在标准归一化中,量子谐振子的特征值由正半整数给出,Hermite 函数为特征函数。因此,它的谱zeta函数基本上是由黎曼zeta函数给出的。量子谐振子(qHO)的热核(或传播者)由梅勒公式给出,分割函数则通过求其迹线得到。一般来说,给定系统的谱zeta函数由其分割函数的梅林变换得到。然而,在非交换谐振子(NCHO)的情况下,热核和分割函数仍然是未知的,尽管人们已经研究了相应谱zeta函数的非定常延续以及在正整数点的特殊值。另一方面,量子拉比模型(QRM)的热核和分区函数的明确公式已经得到,该模型是光与物质相互作用的最简单和最基本的模型,此外还以 NCHO 作为覆盖模型。在本文中,我们提出了一个量子相互作用模型的准分区函数的概念,即如果相应的谱zeta函数可以在整个复平面上进行分形延续,则该模型的准分区函数可以在整个复平面上进行分形延续。qHO 和 QRM 的准分区函数实际上给出了分区函数。假设这一点对 NCHO 成立(目前只是一种猜想),我们就能发现 NCHO 谱的各种有趣性质。此外,尽管我们不能指望量子相互作用模型的谱 zeta 函数有任何函数方程,但我们还是试图寻找正负点的特殊值之间是否存在某种关系。为了寻求这种关系,我们遇到了某些发散级数,它们通过计算分区函数的积分来正式表达赫维茨zeta函数。然后,我们给出了这些发散级数的两种解释:伯累尔求和和由-adic Hurwitz zeta 函数定义的-adically 收敛级数。
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