论文标题

量子过程的实验表征:一种任意有限维度的选择性有效方法

Experimental characterization of quantum processes: a selective and efficient method in arbitrary finite dimension

论文作者

Stefano, Quimey Pears, Perito, Ignacio, Varga, Juan José Miguel, Rebón, Lorena, Iemmi, Claudio

论文摘要

量子系统的时间演变可以以量子过程断层扫描为特征,这是一项复杂的任务,该任务与子系统的数量呈指数缩放。量子通道的完整重建的另一种方法可以从其矩阵描述中选择哪个系数来测量,以及如何准确地减少多项式的资源量。实施此方法的可能性与建立一组完整的互无偏基(MUB)的可能性密切相关,仅当希尔伯特空间的尺寸是素数的力量时,其存在才知道。但是,最近引入了使用最大MUB的张量产品的扩展。在这里,我们明确描述了如何实施该算法以选择性有效地估算出在非prime功率维度中表征量子过程的任何参数,我们首次在维度的Hilbert Space $ d = 6 $中对方法进行了实验验证。那是一个少数空间,没有一个完整的MUB集,但可以将其分解为其他两个尺寸的Hilbert Space的张量产品$ d_1 = 2 $和$ d_2 = 3 $,为此,已知一套完整的Mubs。 $ 6 $维状态以光子波前的离散横向动量进行了编纂。在多功能实验设置中,使用仅相位的空间调制器使用仅使用相的空间调制器对状态的准备和检测阶段进行了动态编程,该设置允许在任何有限的维度中实现该算法。

The temporal evolution of a quantum system can be characterized by quantum process tomography, a complex task that consumes a number of physical resources scaling exponentially with the number of subsystems. An alternative approach to the full reconstruction of a quantum channel allows selecting which coefficient from its matrix description to measure, and how accurately, reducing the amount of resources to be polynomial. The possibility of implementing this method is closely related to the possibility of building a complete set of mutually unbiased bases (MUBs) whose existence is known only when the dimension of the Hilbert space is the power of a prime number. However, an extension of the method that uses tensor products of maximal sets of MUBs, has been introduced recently. Here we explicitly describe how to implement this algorithm to selectively and efficiently estimate any parameter characterizing a quantum process in a non-prime power dimension, and we conducted for the first time an experimental verification of the method in a Hilbert space of dimension $d=6$. That is the small space for which there is no known a complete set of MUBs but it can be decomposed as a tensor product of two other Hilbert spaces of dimensions $D_1=2$ and $D_2=3$, for which a complete set of MUBs is known. The $6$-dimensional states were codified in the discretized transverse momentum of the photon wavefront. The state preparation and detection stages are dynamically programmed with the use of only-phase spatial light modulators, in a versatile experimental setup that allows to implement the algorithm in any finite dimension.

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