2021
DOI: 10.1103/physreva.104.063120
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Noise spectroscopy with a Rydberg ensemble in a hot atomic vapor cell

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Cited by 8 publications
(4 citation statements)
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“…A sub-Doppler spectrum of the 6S 1/2 →6P 3/2 →72S 1/2 Rydberg EIT signal was obtained using counterpropagating excitation beams from the probe and coupling lasers. The typical EIT linewidth measures several tens of megahertz [7,12,28,29], which is considerably larger than the spontaneous emission linewidth of Rydberg states. These spectral broadenings include spontaneous emission broadening of the intermediate levels and power broadening of the coupling laser beam, the latter of which can be converted into two-photon detuning using the EIT scheme, resulting in a velocitydependent residual Doppler effect.…”
Section: Resultsmentioning
confidence: 98%
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“…A sub-Doppler spectrum of the 6S 1/2 →6P 3/2 →72S 1/2 Rydberg EIT signal was obtained using counterpropagating excitation beams from the probe and coupling lasers. The typical EIT linewidth measures several tens of megahertz [7,12,28,29], which is considerably larger than the spontaneous emission linewidth of Rydberg states. These spectral broadenings include spontaneous emission broadening of the intermediate levels and power broadening of the coupling laser beam, the latter of which can be converted into two-photon detuning using the EIT scheme, resulting in a velocitydependent residual Doppler effect.…”
Section: Resultsmentioning
confidence: 98%
“…In principle, auxiliary field dressings can recover the coupling near the homogeneous or spontaneous decay limits in a room-temperature atom ensemble; however, in practice, Rydberg atoms are susceptible to excitation and stray environmental electromagnetic fields. Blackbody radiation can couple adjacent Rydberg states in atom ensembles at room temperature, thereby causing energy shifts or mixing [12,32]. Moreover, optical pumping and polarization introduce polarization broadening of the magnetic quantum number m, which describes vector and tensor polarizabilities [33,34].…”
Section: Resultsmentioning
confidence: 99%
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“…由于低频电场波长较长, 传统滤波放大方 法 往 往 无 法 兼 顾 低 频 电 磁 场 的 高 频 特 性 , 电 场 畸变会导致波形识别不准确、系统动态特性测量困 难等问题 [5] . 近年来, 研究人员提出利用里德伯原子 构建原子天线开展电磁场参数测量 [6][7][8][9][10] , 基于原子 天线的测量方法可以将电磁场的场强测量通过光 谱技术转换到频率测量上, 实现电磁场量值溯源, 因 此原子天线技术广泛应用于电磁场参数测量领域. 里德伯原子是主量子数较大的高激发态原子, 其具有较大的极化率和电偶极矩, 对电磁场十分敏 感 [11,12] .…”
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