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arXiv math-ph/0503013math-phmath.MPquant-ph
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含时奇异量子振子的量子保真度

The quantum fidelity for the time-dependent singular quantum oscillator

M. Combescure

摘要:

在本文中,我们对哈密顿量的时间周期量子谐振子:$$ \hat H\_{g}(t):=\frac{P^2}{2}+ f(t)\frac{Q^2}{2}+\frac{g^2}{Q^2} $$的“量子保真度”(也称为Loscher-Echo)进行了精确的研究,当$f$是$T$ -周期函数,$g$是实常数时,与由$\hat H\_{0}(t)$($g=0$)引起的量子演化进行了比较.参考(初始)状态被认为是Perelomov意义下的任意“广义相干态”。我们表明,在$t=0$附近的时间的平方减少开始,这种量子保真度可能会在无限的时间序列{ $t\_{k}$ }重现到它的初始值1。我们讨论了当哈密顿量$\hat H\_{0}(t)$诱导的经典运动被假定为稳定与不稳定时的结果。量子保真度和经典保真度之间的一个美丽的关系也被证明。

英文摘要:

In this paper we perform an exact study of ``Quantum Fidelity'' (also called Loschmidt Echo) for the time-periodic quantum Harmonic Oscillator of Hamiltonian : $$ \hat H\_{g}(t):=\frac{P^2}{2}+ f(t)\frac{Q^2}{2}+\frac{g^2}{Q^2} $$ when compared with the quantum evolution induced by $\hat H\_{0}(t)$ ($g=0$), in the case where $f$ is a $T$-periodic function and $g$ a real constant. The reference (initial) state is taken to be an arbitrary ``generalized coherent state'' in the sense of Perelomov. We show that, starting with a quadratic decrease in time in the neighborhood of $t=0$, this quantum fidelity may recur to its initial value 1 at an infinite sequence of times {$t\_{k}$}. We discuss the result when the classical motion induced by Hamiltonian $\hat H\_{0}(t)$ is assumed to be stable versus unstable. A beautiful relationship between the quantum and the classical fidelity is also demonstrated.

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