局部量子自旋链淬火的有限时间路径场论微扰方法

Domagoj Kuić, Alemka Knapp, Diana Šaponja-Milutinović
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引用次数: 0

摘要

我们用有限时间路径场理论的微扰方法讨论了以下自旋链中的局部磁场淬火问题:在横向磁场中的 Ising 和 XY 自旋链。它们的共同特点是:i) 通过映射到二次量子化的非相互作用费米子问题,它们是可积分的;ii) 当基态是非能态时(除特殊情况外,有限自旋链都是如此),它可以表示为波哥留布夫费米子真空。如果在有限时间内切换局部磁场扰动,问题就变得不可解,必须通过数值或扰动方法来解决。利用基于投影函数维格纳变换的有限时间路径场理论的形式主义,我们展示了如何:i) 计算淬火链的洛斯赫密特回波中任何阶次扰动的基本 "气泡 "图;ii) 在 "气泡 "图中对铁离子两点迟滞函数的广义施文格-戴森方程进行求和,从而在一定的类比性假设条件下,在广泛的扰动强度范围内实现洛斯赫密特回波扰动展开的求和。我们还进一步讨论了假设的局限性、超越假设的概括以及对其他自旋链的可能概括。
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Finite time path field theory perturbative methods for local quantum spin chain quenches
We discuss local magnetic field quenches using perturbative methods of finite time path field theory in the following spin chains: Ising and XY in a transverse magnetic field. Their common characteristics are: i) they are integrable via mapping to second quantized noninteracting fermion problem; ii) when the ground state is nondegenerate (true for finite chains except in special cases) it can be represented as a vacuum of Bogoliubov fermions. By switching on a local magnetic field perturbation at finite time, the problem becomes nonintegrable and must be approached via numeric or perturbative methods. Using the formalism of finite time path field theory based on Wigner transforms of projected functions, we show how to: i) calculate the basic "bubble" diagram in the Loschmidt echo of a quenched chain to any order in the perturbation; ii) resum the generalized Schwinger-Dyson equation for the fermion two point retarded functions in the "bubble" diagram, hence achieving the resummation of perturbative expansion of Loschmidt echo for a wide range of perturbation strengths under certain analiticity assumptions. Limitations of the assumptions and possible generalizations beyond it and also for other spin chains are further discussed.
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