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Decoherence in the quantum Ising model with transverse dissipative interaction in the strong-coupling regime

机译:在强耦合制度中具有横向耗散相互作用的量子读模型的变阻

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We study the decoherence dynamics of a quantum Ising lattice of finite size with a transverse dissipative interaction, namely, the coupling with the bath is assumed perpendicular to the direction of the spins interaction and parallel to the external magnetic field. In the limit of small transverse field, the eigenstates and spectrum are obtained by a strong-coupling expansion, from which we derive the Lindblad equation in the Markovian limit. At temperature lower than the energy gap and for weak dissipation, the decoherence dynamics can be restricted to take only the two degenerate ground states and the first excited subspace into account. The latter is formed by pairs of topological excitations (domain walls or kinks), which are quantum delocalized along the chain due to the small magnetic field. We find that some of these excited states form a relaxation-free subspace, namely, they do not decay to the ground states.
机译:我们研究了用横向耗散相互作用的有限尺寸的量子刻度晶格的变形动力学,即,垂直于旋转相互作用的方向和平行于外部磁场的耦合与浴槽的联接。 在小横向场的极限中,通过强耦合膨胀来获得特征酯和光谱,从中获得了马尔科夫极限中的Lindblad方程。 在低于能隙和弱化耗散的温度下,可以限制脱机动态,仅考虑两个退化的地面和第一个激发子空间。 后者通过成对的拓扑激发(畴壁或扭结)形成,其由于小磁场而沿着链划分的量子。 我们发现一些这些激发态形成了一种无放松的子空间,即,他们不会腐烂到地面州。

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