Programming an optical lattice interferometer

Lennart Maximilian Seifert , Victor E. Colussi , Michael A. Perlin , Pranav Gokhale , Frederic T. Chong
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Abstract

Programming a quantum device describes the usage of quantum logic gates, agnostic of hardware specifics, to perform a sequence of operations with (typically) a computing or sensing task in mind. Such programs have been executed on gate-based quantum computers, which despite their noisy character, have shown the ability to optimize metrological functions, for example in the generation of spin squeezing and optimization of quantum Fisher information for signals manifesting as spin rotations in a quantum register. However, the qubits of these programmable quantum sensors are tightly spatially confined and therefore suboptimal for enclosing the kinds of large spacetime areas required for performing inertial sensing. In this work, we derive a set of quantum logic gates for a cold atom optical lattice interferometer that manipulates the momentum of atoms. Here, the operations are framed in terms of single qubit operations and mappings between qubit subspaces with internal levels given by the Bloch (crystal) eigenstates of the lattice. We describe how the quantum optimal control method of direct collocation is well suited for obtaining modulation waveforms of an optical lattice to achieve these operations in existing experimental setups.
光栅干涉仪编程
量子设备编程描述了量子逻辑门的使用,不知道硬件细节,执行一系列操作(通常)计算或感知任务。这样的程序已经在基于门的量子计算机上执行,尽管它们具有噪声特征,但已经显示出优化计量功能的能力,例如在自旋压缩的生成和量子费雪信息的优化中,这些信息在量子寄存器中表现为自旋旋转。然而,这些可编程量子传感器的量子位在空间上受到严格限制,因此对于封闭执行惯性传感所需的大时空区域来说不是最佳的。在这项工作中,我们推导了一组用于操纵原子动量的冷原子光学晶格干涉仪的量子逻辑门。在这里,操作是根据单个量子位操作和量子位子空间之间的映射来构建的,量子位子空间具有由晶格的Bloch(晶体)特征态给出的内部水平。我们描述了直接搭配的量子最优控制方法如何非常适合于在现有的实验装置中获得光学晶格的调制波形以实现这些操作。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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