基于玻色-爱因斯坦凝聚光脉冲原子干涉法检验玻恩定则的建议

IF 4.3 Q1 OPTICS
Simon Kanthak, Julia Pahl, Daniel Reiche, Markus Krutzik
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引用次数: 0

摘要

提出了超冷量子气体的光脉冲原子干涉测量方法,并对其进行了数值基准测试,作为验证玻恩规则模方假设的平台。干涉方案是基于双布拉格和单拉曼衍射的组合来诱导玻色-爱因斯坦凝聚体(BECs)中的多径干涉,并分别阻断选定的干涉仪路径。与之前使用宏观材料狭缝和阻挡掩模的测试相比,光学衍射晶格提供了高度的控制,并避免了制造过程中的几何不精确等可能的系统误差。此外,delta-kick准直BECs的亚反冲膨胀率允许制备、区分和选择性地处理原子的外部动量状态。这进一步显示了接近统一的衍射保真度,有利于高对比度干涉测量和高消光的阻挡掩模。反过来,需要考虑原子-原子相互排斥作用引起的非线性相移,我们在多径干涉仪的数值模拟中充分反映了这一点。假设模平方法则成立,根据传统的BEC干涉仪检测了实验不确定度的影响,得到了5.7 × 10−3 ~ 1.8 ×的上界10−3 $5.7\乘以10^{-3}\ \左(1.8\乘以10^{-3}\右)$在100 1000的统计偏差上$100 \ \左($ 1000\右)$迭代一个假设的三阶干涉项。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Proposal for a Bose–Einstein Condensate Based Test of Born's Rule Using Light–Pulse Atom Interferometry

Proposal for a Bose–Einstein Condensate Based Test of Born's Rule Using Light–Pulse Atom Interferometry

Light-pulse atom interferometry with ultra-cold quantum gases is proposed and numerically benchmarked as a platform to test the modulo-square hypothesis of Born's rule. The interferometric protocol is based on a combination of double Bragg and single Raman diffraction to induce multipath interference in Bose–Einstein condensates (BECs) and block selected interferometer paths, respectively. In contrast to previous tests employing macroscopic material slits and blocking masks, optical diffraction lattices provide a high degree of control and avoid possible systematic errors like geometrical inaccuracies from manufacturing processes. In addition, sub-recoil expansion rates of delta-kick collimated BECs allow to prepare, distinguish and selectively address the external momentum states of the atoms. This further displays in close-to-unity diffraction fidelities favorable for both high-contrast interferometry and high extinction of the blocking masks. In return, non-linear phase shifts caused by repulsive atom-atom interactions need to be taken into account, which we fully reflect in our numerical simulations of the multipath interferometer. Assuming that the modulo-square rule holds, the impact of experimental uncertainties is examined in accordance with conventional BEC interferometer to provide an upper bound of 5.7 × 10 3 1.8 × 10 3 $5.7\times 10^{-3} \ \left(1.8\times 10^{-3}\right)$ on the statistical deviation of 100 1000 $100 \ \left(1000\right)$ iterations for a hypothetical third-order interference term.

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