从光学点阵钟到卡西米尔状态下力的测量

P. Wolf, P. Lemonde, A. Lambrecht, S. Bize, A. Landragin, A. Clairon
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引用次数: 47

摘要

作者提出了一个新颖的实验,基于原子被困在宏观表面附近,以研究原子与表面在非常小的距离(0.6至10微米)之间的相互作用。在这个范围内,主导势是表面和原子之间的QED相互作用(卡西米尔-波尔德和范德华)。此外,一些理论模型表明,在与重力相关的新物理中,可能出现亚毫米范围的汤川型势。这篇论文提出了一种与中性原子光学晶格时钟非常相似的设置,但是原子被困在靠近反射镜的晶格位置。然后,不同频率的探测激光脉冲序列被用来制造一个干涉仪,在距离镜子不同距离的原子状态之间(在不同的晶格位置)产生相干叠加。假设原子干涉法测量的最先进的相位差和叠加的持续时间约为0.1s,我们期望能够测量分离状态之间的电位差,不确定度约为10-4Hz。对不同原子(Sr, Yb, Rb, Cs)的系统效应的初步分析表明,在相同的不确定度水平上没有根本的限制效应,但确实影响原子和同位素的选择。基于这些估计,我们预计这样的实验将使原子壁QED相互作用的最佳现有测量提高<2个数量级,同时在100 nm和100 nm之间的新相互作用的最佳现有限制上获得高达4个数量级
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From Optical Lattice Clocks to the Measurement of Forces in the Casimir Regime
The authors propose a novel experiment based on atoms trapped close to a macroscopic surface, to study the interactions between the atoms and the surface at very small separations (0.6 to 10 mum). In this range the dominant potential is the QED interaction (Casimir-Polder and Van der Waals) between the surface and the atom. Additionally, several theoretical models suggest the possibility of Yukawa type potentials with sub-mm range, arising from new physics related to gravity. The paper proposes a set-up very similar to neutral atom optical lattice clocks, but with the atoms trapped in lattice sites close to the reflecting mirror. A sequence of pulses of the probe laser at different frequencies is then used to create an interferometer with a coherent superposition between atomic states at different distances from the mirror (in different lattice sites). Assuming atom interferometry state of the art measurement of the phase difference and a duration of the superposition of about 0.1s we expect to be able to measure the potential difference between separated states with an uncertainty of about 10-4Hz. A preliminary analysis of systematic effects for different atoms (Sr, Yb, Rb, Cs) indicates no fundamentally limiting effect at the same level of uncertainty, but does influence the choice of atom and isotope. Based on those estimates, we expect that such an experiment would improve the best existing measurements of the atom-wall QED interaction by <2 orders of magnitude, whilst gaining up to 4 orders of magnitude on the best present limits on new interactions in the range between 100 nm and 100mum
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