玻色-爱因斯坦凝聚气体中激发粒子态占据数的多体涨落量子优越性
Quantum supremacy of the many-body fluctuations in the occupations of the excited particle states in a Bose-Einstein-condensed gas
AI总结:
本研究推导了BEC气体粒子占据数联合分布的特征函数公式与Hafnian主定理,提出多量子比特BEC阱原子玻色采样模型,证明其多体涨落计算为#P难,可用于展示多体相互作用系统的量子优越性。
摘要:
我们推导出了BEC(玻色-爱因斯坦凝聚)气体中粒子占据数联合概率分布的特征函数(傅里叶变换)的通用解析公式,以及推广了著名的MacMahon积和式主定理的Hafnian主定理。我们提出了一个颇具吸引力的模型——由一组量子比特势阱构成的多量子比特BEC阱,并讨论了这种原子玻色采样系统与光子玻色采样系统相比的特性。最后,BEC阱中的多体涨落过程的计算属于#P难问题,可作为证明多体相互作用系统相较于经典模拟器具有量子优越性的基础。
英文摘要:
We find a universal analytic formula for a characteristic function (Fourier transform) of a joint probability distribution for the particle occupation numbers in a BEC gas and the Hafnian Master Theorem generalizing the famous Permanent Master Theorem of MacMahon. We suggest an appealing model, a multi-qubit BEC trap formed by a set of qubit potential wells, and discuss specifics of such an atomic boson-sampling system vs a photonic one. Finally, the process of many-body fluctuations in a BEC trap is #P-hard for computing. It could serve as a basis for demonstrating quantum supremacy of the many-body interacting systems over classical simulators.
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。