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arXiv math-ph/0002010math-phmath.MPmath.SP
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亏格为零的可积量子映射的能级间隔

Level Spacings for Integrable Quantum Maps in Genus Zero

Steve Zelditch

摘要:

研究了2-球面上某些可积量子映射的本征值对关联问题。经典映射是完全Morse函数的Hamilton流的时间1映射。量子化是两个复变量的N次齐次全纯多项式空间上的酉算子。单位圆上有N个本征相位,对相关问题是确定本征相位之间的间距在平均能级间距长度尺度上的分布。Berry-Tabor猜想认为,对于一般的可积系统,当N趋于无穷大时,间距分布应趋于泊松(均匀)极限。在本文及其附录中,我们证明了这一猜想的一个弱形式:我们定义了一个大类的两个参数的可积哈密顿族,并证明了几乎所有的元素,每个家庭的极限对关联函数是泊松。在本文中,我们采取的限制沿一个稍微稀疏的子序列的N的;在附录中,我们采取切萨罗手段沿全重。

英文摘要:

We consider the eigenvalue pair correlation problem for certain integrable quantum maps on the 2-sphere. The classical maps are time one maps of Hamiltonian flows of perfect Morse functions. The quantizations are unitary operators on spaces of homogeneous holomorphic polynomials of degree N in two complex variables. There are N eigenphases on the unit circle and the pair correlation problem is to determine the distribution of spacings between the eigenphases on the length scale of the mean level spacing. The Berry-Tabor conjecture says that for generic integrable systems, the spacings distribution should tend to the Poisson (uniform) limit as N tends to infinity. In this paper and in its addendum we prove a somewhat weak form of this conjecture: We define a large class of two parameter families of integrable Hamiltonians, and prove that for almost all elements of each family the limit pair correlation function is Poisson. In this paper, we take the limit along a slightly sparse subsequence of N's; in the addendum we take Cesaro means along the full seuqence.

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