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arXiv quant-ph/0506094quant-ph
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赝厄米量子力学在具有连续散射态的PT对称哈密顿量中的应用

Application of Pseudo-Hermitian Quantum Mechanics to a PT-Symmetric Hamiltonian with a Continuum of Scattering States

Ali Mostafazadeh

摘要:

我们将在伪厄米量子力学框架内发展起来的方法推广到研究由具有连续实谱的虚PT对称势v(x)描述的么正量子系统.对于这个潜在的,最近已被使用,在光势的背景下,用于模拟传播的电磁波在波导中的半场增益和吸收介质,我们给出了一个微扰的物理希尔伯特空间,可观的,本地化的状态,和等效的厄米哈密顿。忽略非厄米性参数zeta中的三阶或更高阶项,我们证明了等价厄米哈密顿量具有$\frac{p^2}{2m}+\frac{ζ^2}{2}\sum_{n=0}^\infty\{α_n(x),p^{2n}\}$的形式,其中$α_n(x)$在比$v(x)$的支持大三倍的区间之外消失,即,在2/3的物理相互作用区域中,电势$v(x)$相同地消失。我们提供了一个物理解释,这种不寻常的行为和评论的经典极限的系统。

英文摘要:

We extend the application of the techniques developed within the framework of the pseudo-Hermitian quantum mechanics to study a unitary quantum system described by an imaginary PT-symmetric potential v(x) having a continuous real spectrum. For this potential that has recently been used, in the context of optical potentials, for modelling the propagation of electromagnetic waves travelling in a wave guide half and half filed with gain and absorbing media, we give a perturbative construction of the physical Hilbert space, observables, localized states, and the equivalent Hermitian Hamiltonian. Ignoring terms of order three or higher in the non-Hermiticity parameter zeta, we show that the equivalent Hermitian Hamiltonian has the form $\frac{p^2}{2m}+\frac{ζ^2}{2}\sum_{n=0}^\infty\{α_n(x),p^{2n}\}$ with $α_n(x)$ vanishing outside an interval that is three times larger than the support of $v(x)$, i.e., in 2/3 of the physical interaction region the potential $v(x)$ vanishes identically. We provide a physical interpretation for this unusual behavior and comment on the classical limit of the system.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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