连续参数不可积系统中的量子经典对应

T. Takami
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引用次数: 2

摘要

研究了具有连续参数的不可积系统中的量子经典对应。在以展弦比为参数的体育场台球中,我们证明了特征值的参数运动的斜率主要是由周期轨道长度对参数的一阶导数引起的。我们还提出了系统连续变化中的伤痕波函数的观点。自从在体育场台球中发现了疤痕以来,许多作者对各种系统中疤痕的性质进行了数值研究。一些理论研究试图解释波函数在不稳定周期轨道(PO)上的额外积累。虽然这些工作似乎在数值和理论上都证实了疤痕的存在,但尚未给出不可积系统中单个特征态的半经典理论。研究单个特征态的困难是由于与其他态的强相互作用。排斥相互作用的起源已经被许多作者研究过,并且与经典运动中的混沌行为有关。当我们改变哈密顿量中的一个参数时,众所周知,不可积系统的特征值由于相互作用而显示出许多避免交叉。这种相互作用的明确表示是由关卡动力学给出的。>和能级的运动可以用一个完全可积的经典哈密顿量来描述。引入水平曲率,即特征值对参数的二阶导数来表征特征值的参数化性质,并推导了分布的大曲率尾的表达式。8>通过数值计算在各种系统中检验了大曲率下的普遍行为。另一方面,用数值方法发现了小曲率的非普适性。Zakrzewski和Delande11提出,小曲率的差异可以用来对不同系统的疤痕程度进行分类。本文以长径比为参数,考虑了经典的运动特征值与运动特征值的关系。在§2中,我们研究了连续改变参数时PO的性质。我们专注于PO的连续性,并计算了
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Quantum Classical Correspondence in Nonintegrable Systems with Continuous Parameter
We study quantum classical correspondence in nonintegrable systems with a continuous parameter. In a stadium billiard with an aspect ratio as a parameter, we show that the slope of the parametric motion of eigenvalues is mainly due to the first derivative of periodic orbit length with respect to the parameter. We also present a viewpoint for scarred wavefunctions in a continuous change of the systems. Since the discovery of scars 1 > in a stadium billiard/> a number of authors have studied properties of scars numerically in various systems.3> Several theoretical studies4 >,s> have tried to explain the extra accumulation of the wave function on an unstable periodic orbit (PO). Although these works seemed to confirm the existence of scars both numerically and theoretically, the semiclassical theory for individual eigenstates in nonintegrable systems has not been given yet. The difficulty in the investigation for the individual eigenstates is due to the strong interaction with other states. The origin of the repulsive interaction has been studied by many authors, and was related to chaotic behavior in the classical motion. 6> When we change a parameter in the Hamiltonian, it is well known that eigenvalues of nonintegrable systems show a number of avoided crossings due to the interaction. The definite representation for the interaction was given by the level dynamics,?> and the motion of levels was shown to be described by a classical Hamiltonian with complete integrability. The curvature of levels, i.e. the second derivative of eigenvalues with respect to the parameter, have been introduced to characterize the parametric property of eigenvalues, and the expressions for the large curvature tail of the distribution have been derived. 8> The universal behavior in large curvatures is checked in various systems by numerical calculations. 9 > On the other hand, the nonuniversal behavior of small curvatures was discovered numerically. 10> Zakrzewski and Delande11> suggest that the discrepancy in small curvatures can be used to classify the degree of scarring in different systems. In this paper, we consider the relation between classical PO's and the parametric motion of eigenvalues of the stadium billiard with an aspect ratio as a parameter. In § 2, we study properties of PO's when we change the parameter continuously. We concentrate on the continuity of the PO's and calculate the first derivative of the
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