基于有限域的离散相空间
Discrete phase space based on finite fields
摘要:
原始的维格纳函数提供了一种在相空间中表示具有连续自由度的系统的量子态的方法。维格纳函数也已经被开发用于离散量子系统,一个流行的版本被定义在具有N个正交态的系统的2N × 2N离散相空间上。在这里,我们研究了另一类离散维格纳函数,在该领域的实数,标签轴的连续相空间被替换为一个有限域有N个元素。存在这样一个场当且仅当N是素数的幂;因此我们的公式只能直接应用于状态空间维数取这样一个值的系统。虽然这个条件看起来很有限,但我们注意到,任何基于量子比特的量子计算机都符合这个条件,因此可以在我们的方案中使用。我们的N × N相空间的几何形状也自然地导致一种方法,构造一个完整的一组N+1相互无偏基地的状态空间。
英文摘要:
The original Wigner function provides a way of representing in phase space the quantum states of systems with continuous degrees of freedom. Wigner functions have also been developed for discrete quantum systems, one popular version being defined on a 2N x 2N discrete phase space for a system with N orthogonal states. Here we investigate an alternative class of discrete Wigner functions, in which the field of real numbers that labels the axes of continuous phase space is replaced by a finite field having N elements. There exists such a field if and only if N is a power of a prime; so our formulation can be applied directly only to systems for which the state-space dimension takes such a value. Though this condition may seem limiting, we note that any quantum computer based on qubits meets the condition and can thus be accommodated within our scheme. The geometry of our N x N phase space also leads naturally to a method of constructing a complete set of N+1 mutually unbiased bases for the state space.
机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。