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Non-equilibrium spin-boson model: Counting statistics and the heat exchange fluctuation theorem

机译:非平衡自旋玻色子模型:计数统计和热交换波动定理

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摘要

We focus on the non-equilibrium two-bath spin-boson model, a toy model for examining quantum thermal transport in many-body open systems. Describing the dynamics within the noninteracting-blip approximation equations, applicable, e.g., in the strong system-bath coupling limit and/or at high temperatures, we derive expressions for the cumulant generating function in both the Markovian and non-Markovian limits by energy-resolving the quantum master equation of the subsystem. For a Markovian bath, we readily demonstrate the validity of a steady-state heat exchange fluctuation theorem. In the non-Markovian limit a "weaker "symmetry relation generally holds, a general outcome of microreversibility. We discuss the reduction of this symmetry relation to the universal steady-state fluctuation theorem. Using the cumulant generating function, an analytic expression for the heat current is obtained. Our results establish the validity of the steady-state heat exchange fluctuation theorem in quantum systems with strong system-bath interactions. From the practical point of view, this study provides tools for exploring transport characteristics of the two-bath spin-boson model, a prototype for a nonlinear thermal conductor.
机译:我们关注于非平衡两浴自旋玻色子模型,该模型用于检查多体开放系统中的量子热传输。描述非相互作用斑点近似方程式中的动力学,例如适用于强系统-浴耦合极限和/或高温,我们通过能量推导得出马尔可夫和非马尔可夫极限中累积量生成函数的表达式。求解子系统的量子主方程。对于马尔可夫浴,我们很容易地证明了稳态热交换波动定理的有效性。在非马尔可夫极限中,“较弱”的对称关系通常成立,这是微观可逆性的普遍结果。我们讨论将这种对称关系简化为普遍稳态波动定理。使用累积量生成函数,可以获得热电流的解析表达式。我们的结果建立了稳态热交换涨落定理在强系统-浴相互作用的量子系统中的有效性。从实用的角度来看,本研究提供了工具,用于探索两浴自旋玻色子模型(非线性热导体的原型)的传输特性。

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