Dipole-dipole interactions between helium atoms in Rydberg-Stark states withprincipal quantum number $n=53$ and approximately linear Stark energy shifts,resulting from induced electric dipole moments of approximately 7900 D, havebeen investigated experimentally. The experiments were performed in pulsedsupersonic metastable helium beams, with particle number densities of up to$\sim10^9$ cm$^{-3}$. In the presence of amplitude-modulated, radio-frequencyelectric fields, changes in the spectral intensity distributions associatedwith the transitions to these states that are attributed to dipole-dipoleinteractions within the ensembles of excited atoms have been observed. Theexperimental results are in excellent agreement with calculations of theRydberg energy level structure carried out using Floquet methods, andexcitations shared by up to 4 atoms. The use of these Rydberg-Stark states assensors for non-resonant broadband radio-frequency electrical noise is alsodiscussed.
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机译:实验研究了基本量子数$ n = 53 $的Rydberg-Stark态中氦原子之间的偶极-偶极相互作用,以及大约7900 D的感应电偶极矩引起的近似线性Stark能量位移。实验是在脉冲超音速亚稳氦气束中进行的,粒子数密度高达$ \ sim10 ^ 9 $ cm $ ^ {-3} $。在存在振幅调制的射频电场的情况下,已经观察到光谱强度分布的变化,这些变化与归因于激发原子集合内的偶极-偶极相互作用的这些状态的跃迁有关。实验结果与使用Floquet方法进行的里德伯格能级结构的计算以及最多4个原子共享的激发非常吻合。还讨论了使用这些Rydberg-Stark状态作为非谐振宽带射频电噪声的传感器。
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