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首页> 外文期刊>New journal of physics >Quantum circuit dynamics via path integrals: Is there a classical action for discrete-time paths?
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Quantum circuit dynamics via path integrals: Is there a classical action for discrete-time paths?

机译:通过路径积分的量子电路动力学:离散时间路径有经典的作用吗?

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摘要

It is straightforward to compute the transition amplitudes of a quantum circuit using the sum-over-paths methodology when the gates in the circuit are balanced, where a balanced gate is one for which all non-zero transition amplitudes are of equal magnitude. Here we consider the question of whether, for such circuits, the relative phases of different discrete-time paths through the configuration space can be defined in terms of a classical action, as they are for continuous-time paths. We show how to do so for certain kinds of quantum circuits, namely, Clifford circuits where the elementary systems are continuous-variable systems or discrete systems of odd-prime dimension. These types of circuit are distinguished by having phase-space representations that serve to define their classical counterparts. For discrete systems, the phase-space coordinates are also discrete variables. We show that for each gate in the generating set, one can associate a symplectomorphism on the phase-space and to each of these one can associate a generating function, defined on two copies of the configuration space. For discrete systems, the latter association is achieved using tools from algebraic geometry. Finally, we show that if the action functional for a discrete-time path through a sequence of gates is defined using the sum of the corresponding generating functions, then it yields the correct relative phases for the path-sum expression. These results are likely to be relevant for quantizing physical theories where time is fundamentally discrete, characterizing the classical limit of discrete-time quantum dynamics, and proving complexity results for quantum circuits.
机译:当电路中的门处于平衡状态时,使用路径总和方法计算量子电路的跃迁幅度是很简单的,其中平衡的门是所有非零跃迁幅度都相等的幅度。在这里,我们考虑的问题是,对于此类电路,是否可以通过经典操作来定义通过配置空间的不同离散时间路径的相对相位,就像连续时间路径一样。我们展示了如何对某些种类的量子电路(即Clifford电路)执行此操作,其中基本系统是连续变数系统或奇数维的离散系统。这些类型的电路的特征在于具有相空间表示形式,用于定义其经典对应形式。对于离散系统,相空间坐标也是离散变量。我们表明,对于生成集中的每个门,可以在相位空间上关联辛同构,并且对于每个门可以关联在配置空间的两个副本上定义的生成函数。对于离散系统,后者的关联是使用代数几何中的工具实现的。最后,我们表明,如果使用相应生成函数的总和来定义通过一系列门的离散时间路径的动作函数,则它会为路径和表达式产生正确的相对相位。这些结果可能与量化时间根本上是离散的物理理论,表征离散时间量子动力学的经典极限以及证明量子电路的复杂性结果有关。

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