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Discrete time quantum walk model for single and entangled particles to retain entanglement in coin space

机译:单个和纠缠粒子的离散时间量子行走模型   保留硬币空间中的纠缠

摘要

In most widely discussed discrete time quantum walk model, after everyunitary shift operator, the particle evolves into the superposition of positionspace and settles down in one of its basis states, loosing entanglement in thecoin space in the new position. The Hadamard operation is applied to let theparticle to evolve into the superposition in the coin space and the walk isiterated. We present a model with a additional degree of freedom for theunitary shift operator $U^{\prime}$. The unitary operator with additionaldegree of freedom will evolve the quantum particle into superposition ofposition space retaining the entanglement in coin space. This eliminates theneed for quantum coin toss (Hadamard operation) after every unitarydisplacement operation as used in most widely studied version of the discretetime quantum walk model. This construction is easily extended to a multipleparticle quantum walk and in this article we extend it for a pair of particlesin pure state entangled in coin degree of freedom by simultaneously subjectingit to a pair of unitary displacement operators which were constructed forsingle particle. We point out that unlike for single particle quantum walk,upon measurement of its position after $N$ steps, the entangled particles arefound together with 1/2 probability and at different positions with 1/2probability. This can act as an advantage in applications of the quantum walk.A special case is also treated using a complex physical system such as, interspecies two-particle entangled Bose-Einstein condensate, as an example.
机译:在讨论最广泛的离散时间量子游走模型中,每个单位移位算子之后,粒子演化为位置空间的叠加并以其基态之一沉降,从而使新空间中的硬币空间失去纠缠。应用Hadamard运算使粒子在硬币空间中演化为叠置,并进行遍历。我们为with移算子$ U ^ {\ prime} $提出了一个附加的自由度模型。具有附加自由度的unit算子将把量子粒子演化为位置空间的叠加,从而保持纠缠在硬币空间中。这消除了在离散时间量子游走模型的最广泛研究版本中使用的每个单位位移操作之后进行量子硬币抛掷(Hadamard操作)的需要。这种构造很容易扩展到多粒子量子行走,在本文中,我们通过同时对一对构造为单个粒子的constructed位移算子进行处理,将其扩展为纠缠于硬币自由度的一对纯态粒子。我们指出,与单粒子量子行走不同,在$ N $步长后测量其位置时,纠缠的粒子与1/2概率一起被发现,而在不同位置则具有1/2概率。这可以在量子走动的应用中发挥优势。特殊情况也可以通过复杂的物理系统处理,例如种间两粒子纠缠的玻色-爱因斯坦凝聚物。

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  • 作者

    Chandrashekar, C. M.;

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  • 年度 2006
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  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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