Energy--Level Statistics of Model Quantum Systems: Universality and Scaling in a Lattice--Point Problem
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We investigate the statistics of the number $N(R,S)$ of lattice points, $n\in \Z^2$, in a ``random'' annular domain $\Pi(R,w)=\,(R+w)A\,\setminus RA$, where $R,w >0$. Here $A$ is a fixed convex set with smooth boundary and $w$ is chosen so that the area of $\Pi (R,w)$ is $S$. The randomness comes from $R$ being taken as random ( with a smooth denisity ) in some interval $[c_1T,c_2T]$, $c_2>c_1>0$. We find that in the limit $T\to\infty $ the variance and distribution of $\De N=N(R;S)-S$ depends strongly on how $S$ grows with $T$. There is a saturation regime $S/T\to\infty$, as $T\to\infty$ in which the fluctuations in $\Delta N$ coming from the two boundaries of $\Pi $, are independent. Then there is a scaling regime, $S/T\to z$, $0<z<\infty $ in which the distribution depends on $z$ in an almost periodic way going to a Gaussian as $z\to\ 0$. The variance in this limit approaches $z$ for ``generic'' $A$ but can be larger for ``degenerate'' cases. The former behavior is what one would expect from the Poisson limit of a distribution for annuli of finite area.
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