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Det-Det correlations for quantum maps: Dual pair and saddle-point analyses

机译:量子图的Det-Det相关性:双对和鞍点分析

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摘要

An attempt is made to clarify the ballistic nonlinear sigma model formalism recently proposed for quantum chaotic systems, by looking at the spectral determinant Z(s)=Det(1-sU) for quantized maps Uis an element ofU(N), and studying the correlator omega(U)(s)=integraldthetaparallel toZ(e(itheta)s)parallel to(2). By identifying U(N) as one member of a dual pair acting in the spinor representation of Spin(4N), the expansion of omega(U)(s) in powers of s(2) is shown to be a decomposition into irreducible characters of U(N). In close analogy with the ballistic nonlinear sigma model, a coherent-state integral representation of omega(U)(s) is developed. For generic U this integral has ((2N)(N)) saddle points and the leading-order saddle-point approximation turns out to reproduce omega(U)(s) exactly, up to a constant factor. This miracle is explained by interpreting omega(U)(s) as a character of U(2N), and arguing that the leading-order saddle-point result corresponds to the Weyl character formula. Unfortunately, the Weyl decomposition behaves nonsmoothly in the semiclassical limit N-->infinity, and to make further progress some additional averaging needs to be introduced. Several schemes are investigated, including averaging over basis states and an "isotropic" average. The saddle-point approximation applied in conjunction with these schemes is demonstrated to give incorrect results in general, one notable exception being a semiclassical averaging scheme, for which all loop corrections vanish identically. As a side product of the dual pair decomposition with isotropic averaging, the crossover between the Poisson and CUE limits is obtained. (C) 2002 American Institute of Physics. [References: 33]
机译:通过查看量化映射图的频谱决定因素Z(s)= Det(1-sU)Uis是U(N)的一个元素,并研究了量子混沌系统,试图澄清最近为量子混沌系统提出的弹道非线性sigma模型形式主义。相关器ω(U)(s)=与θ(e(itheta)s)平行于(2)的积分θ。通过将U(N)识别为以Spin(4N)的自旋表示表示的双对中的一个成员,以s(2)的幂表示的omega(U)的展开被显示为分解为不可约性的U(N)。与弹道非线性sigma模型非常相似,开发了ω(U)的相干态积分表示。对于泛型U,此积分具有((2N)(N))个鞍点,并且导数阶鞍点近似值可精确地再现ω(U),直至恒定因子为止。通过将omega(U)解释为U(2N)的字符,并辩称前导鞍点结果与Weyl字符公式相对应,可以解释此奇迹。不幸的是,Weyl分解在半经典极限N-> infinity中的表现不平滑,并且为了取得进一步的进展,还需要引入一些附加的平均数。研究了几种方案,包括对基态求平均和“各向同性”平均值。结合这些方案应用的鞍点近似值通常会给出不正确的结果,一个值得注意的例外是半经典平均方案,对于该方案,所有环路校正均会消失。作为具有各向同性平均的双对分解的副产物,获得了泊松极限和CUE极限之间的交叉。 (C)2002美国物理研究所。 [参考:33]

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