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Laser & Optoelectronics Progress

Optimization of Buffer Gas Compositions in Atomic Vapor Cell for Coherent Population Trapping Atomic Clock

李云超 Yunchao Li, 胡旭文 Xuwen Hu, 张璐 Lu Zhang, 刘召军 Zhaojun Liu, 张开放 Kaifang Zhang, 牟仕浩 Shihao Mou, 闫树斌 Shubin Yan, 张彦军 Yanjun Zhang

Published Jan 1, 2019• 0 citations
Publisher
DOI
10.3788/lop56.120201

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Bulletin of the American Physical Society•Oct 30, 2008•1 citation
We report on the characterization of Cs vapor microfabricated cells filled with a Ne-He buffer gas mixture using coherent population trapping (CPT) spectroscopy. The temperature dependence of the Cs clock frequency is found to be canceled at the first order around a so-called inversion temperature higher than 80°C whose value depends on the buffer gas partial pressure ratio. This buffer gas mixture could be well-adapted for the development of miniature atomic clocks devoted to be used in specific applications such as defense and avionic systems with high operating temperature environment (typically higher than 85°C). This solution suggests an alternative to buffer gas mixtures generally used in optically-pumped vapor cell atomic clocks.
We present a pair of phase-locked lasers with a 9.2-GHz frequency difference through the injection locking of a master laser to the RF-modulation sideband of a slave diode laser. Using this laser system, a coherent population trapping (CPT) signal with a typical linewidth of ∼ 182 Hz is obtained in a cesium vapor cell filled with 30 Torr (4 kPa) of neon as the buffer gas. We investigate the influence of the partial pressure of the neon buffer gas on the CPT linewidth, amplitude, and frequency shift. The results may offer some references for CPT atomic clocks and CPT atomic magnetometers.
The goal of this project is to optimize parameters of a prototype atomic clock to achieve the best Allan variance. We have established a prototype atomic clock using coherent population trapping (CPT) by creating a laser system to lock the laser’s frequency to an atomic resonance in rubidium and utilized radiofrequency (rf) modulation to create a sideband and carrier comb. With the system assembled, we have achieved our best Allan variance of 4 × 10−10 for a 15 torr Neon buffer gas cell, but have changed to a 5 torr Neon buffer gas cell to decrease the Allan variance.