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arXiv quant-ph/0402051quant-ph
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时间约束与n-量子比特正则分解

Time Reversal and n-qubit Canonical Decompositions

Stephen S. Bullock, Gavin K. Brennen, Dianne P. O'Leary

摘要:

对于n是偶数个量子比特和v是酉演化,酉群的矩阵分解v=k1 a k2是明确可计算的,并且允许研究并发纠缠单调的动力学。该并发正则分解(CCD)的边因子k1和k2是并发对称的,因此动力学问题归结为对因子a的考虑。在这项工作中,我们提供了一个显式的数值算法计算v=k1 k2为n奇数。此外,在奇数情况下,我们将单调性提升为双参数函数,从而允许奇数量子比特中的并发动力学理论。一般化也可以使用CCD来研究,再次导致大多数酉的最大并发能力。关键的技术是考虑自旋翻转作为一个时间反演对称运营商在维格纳的公理化,原来的CCD推导可以重述完全在这个时间反演。在途中,我们观察到Kramers的非简并性:任何时间反演对称n-量子比特哈密顿量的非简并本征态的存在要求(i)n偶数和(ii)所述本征态的最大并发。我们提供了如何应用这项工作的例子来研究自旋链哈密顿纠缠的运动学和动力学。

英文摘要:

For n an even number of qubits and v a unitary evolution, a matrix decomposition v=k1 a k2 of the unitary group is explicitly computable and allows for study of the dynamics of the concurrence entanglement monotone. The side factors k1 and k2 of this Concurrence Canonical Decomposition (CCD) are concurrence symmetries, so the dynamics reduce to consideration of the a factor. In this work, we provide an explicit numerical algorithm computing v=k1 a k2 for n odd. Further, in the odd case we lift the monotone to a two-argument function, allowing for a theory of concurrence dynamics in odd qubits. The generalization may also be studied using the CCD, leading again to maximal concurrence capacity for most unitaries. The key technique is to consider the spin-flip as a time reversal symmetry operator in Wigner's axiomatization; the original CCD derivation may be restated entirely in terms of this time reversal. En route, we observe a Kramers' nondegeneracy: the existence of a nondegenerate eigenstate of any time reversal symmetric n-qubit Hamiltonian demands (i) n even and (ii) maximal concurrence of said eigenstate. We provide examples of how to apply this work to study the kinematics and dynamics of entanglement in spin chain Hamiltonians.

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