Switching global correlations on and off in a many-body quantum state by tuning local entanglement

Colin Benjamin, Aditya Dash
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Abstract

A quantum many-body state built on a classical 1D Ising model with locally entangled qubits is considered. This setup can model an infinite-player quantum Prisoner's dilemma game with each site representing two entangled players (or qubits). The local entanglement $\gamma$ between two qubits placed on a site in the 1D Ising model and classical coupling between adjacent sites of the Ising model has an apposite influence on qubits. It points to a counter-intuitive situation wherein local entanglement at a site can exactly cancel global correlations, signaling an artificial quantum many-body state wherein, by locally tuning the entanglement at a particular site, one can transition from a strongly correlated quantum state to an uncorrelated quantum state and then to a correlated classical state. In other words, we can simulate a state similar to a Type II superconducting state via local tuning of entanglement in a 1D Ising chain with entangled qubits.
通过调整局部纠缠,在多体量子态中打开和关闭全局相关性
考虑了建立在具有局部纠缠量子比特的经典一维Ising模型上的量子多体态。这种设置可以模拟一个无限玩家的量子囚徒困境游戏,每个站点代表两个纠缠的玩家(或量子比特)。放置在一维Ising模型中一个位置上的两个量子位之间的局部纠缠$\gamma$和ising模型中相邻位置之间的经典耦合对量子位有相应的影响。它指出了一种反直觉的情况,在这种情况下,一个位置的局部纠缠可以精确地抵消全局相关性,表明人工量子多体状态,其中,通过局部调整特定位置的纠缠,可以从强相关的量子态过渡到不相关的量子态,然后再过渡到相关的经典态。换句话说,我们可以通过在具有纠缠量子比特的1DIsing链中局部调谐纠缠来模拟类似于II型超导状态的状态。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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