首页> 外文期刊>Physical Review, A. Atomic, molecular, and optical physics >Optical frequency measurements of 6s S-2(1/2)-6p P-2(1/2) (D-1) transitions in Cs-133 and their impact on the fine-structure constant
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Optical frequency measurements of 6s S-2(1/2)-6p P-2(1/2) (D-1) transitions in Cs-133 and their impact on the fine-structure constant

机译:Cs-133中6s S-2(1/2)-6p P-2(1/2)(D-1)跃迁的光频率测量及其对精细结构常数的影响

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High resolution laser spectroscopy of the 6s S-2(1/2)-> 6p P-2(1/2) transition (D-1 line) in neutral Cs-133 is performed in a highly collimated thermal atomic beam by use of a femtosecond laser frequency comb and narrow-linewidth diode laser. The diode laser is offset locked to a single frequency component of the femtosecond laser frequency comb and probes the optical transitions between selected pairs of ground-state and excited-state hyperfine components. A photodiode detects the excited-state decay fluorescence, and a computerized data acquisition system records the signal. The Doppler shift is eliminated by orienting the laser beam in a direction perpendicular to the atomic beam to within a precision of 5x10(-6) rad. Optical frequencies for all four pairs of hyperfine components are measured independently, from which the D-1 line centroid and excited-state hyperfine splitting are obtained by least-squares minimization with the ground-state splitting as a fixed constraint. We find the D-1 line centroid to be f(D1)=335 116 048 748.1(2.4) kHz, and the 6p P-2(1/2) state hyperfine splitting to be 1 167 723.6(4.8) kHz. These results, in combination with the results of an atom interferometry experiment by Wicht [Phys. Scripta T 102, 82 (2002)], are used to calculate a new value for the fine-structure constant.
机译:中性Cs-133中6s S-2(1/2)-> 6p P-2(1/2)跃迁(D-1线)的高分辨率激光光谱是在高度准直的热原子束中进行的飞秒激光频率梳和窄线宽二极管激光。二极管激光器偏移锁定到飞秒激光器频率梳的单个频率分量,并探测选定的成对的基态和激发态超精细分量之间的光学跃迁。光电二极管检测激发态衰减荧光,计算机数据采集系统记录该信号。通过将激光束沿垂直于原子束的方向定向到5x10(-6)rad的精度内,可以消除多普勒频移。独立测量所有四对超精细分量的光频率,通过最小二乘最小化以基态分裂为固定约束,从中获得D-1线质心和激发态超精细分裂。我们发现D-1线质心为f(D1)= 335 116 048 748.1(2.4)kHz,6p P-2(1/2)状态超精细分裂为1 167 723.6(4.8)kHz。这些结果与Wicht的原子干涉实验结果[Phys。 Scripta T 102,82(2002)],用于计算精细结构常数的新值。

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