scholarly journals Two-photon Optical Frequency Reference with Active ac Stark Shift Cancellation

2018 ◽  
Vol 10 (1) ◽  
Author(s):  
V. Gerginov ◽  
K. Beloy
1995 ◽  
Vol 66 (2) ◽  
pp. 955-960 ◽  
Author(s):  
C. T. Taylor ◽  
M. Notcutt ◽  
D. G. Blair

2004 ◽  
Author(s):  
Mark D. Plimmer ◽  
Thomas Badr ◽  
Stephane Guerandel ◽  
Yann Louyer ◽  
Sylvestre Challemel du Rozier ◽  
...  

1993 ◽  
Vol 102 (5-6) ◽  
pp. 432-438 ◽  
Author(s):  
F. Nez ◽  
F. Biraben ◽  
R. Felder ◽  
Y. Millerioux

2021 ◽  
Vol 19 (2) ◽  
pp. 025201
Author(s):  
Ning Liu ◽  
Sandan Wang ◽  
Jinpeng Yuan ◽  
Lirong Wang ◽  
Liantuan Xiao ◽  
...  

Abstract We experimentally investigate the 6S 1/2–8S 1/2 two-photon transition in cesium vapor by a single laser. A blue (455.5 and 459.3 nm) fluorescence signal is observed as a result of 822.5 nm laser beams illuminating the Cs vapor with a counter-propagating configuration. The dependences of the fluorescence intensity on the polarization combinations of the laser beams, laser power and vapor temperature are studied to obtain optimal experimental parameters. The frequency difference between the two hyperfine components of 4158 (7) MHz is measured with a Fabry–Perot interferometer as a frequency reference. Such a large spectral isolation and the insensitivity to the Earth’s magnetic field enable the 6S 1/2–8S 1/2 transition to be a stable frequency standard candidate for a frequency-doubled 1644 nm laser in the U-band window for quantum telecommunication.


Author(s):  
U. Johann ◽  
T. Schuldt ◽  
K. Döringshoff ◽  
E. Kovalchuk ◽  
J. Pahl ◽  
...  

2011 ◽  
Vol 107 (22) ◽  
Author(s):  
Qun-Feng Chen ◽  
Andrei Troshyn ◽  
Ingo Ernsting ◽  
Steffen Kayser ◽  
Sergey Vasilyev ◽  
...  

2019 ◽  
Vol 9 (5) ◽  
pp. 921
Author(s):  
Haoyuan Lu ◽  
Jianxiao Leng ◽  
Jianye Zhao

We demonstrated the observation of cold rubidium atom two-photon transition excitation by a fiber optical frequency comb. In addition to this, we optimized the repetition rate of optical frequency comb to enhance two-photon intensity by controlling cavity length and pump source of optical comb. This technique can fine tune repetition rate to corresponding stepwise two-photon transition resonance frequency and improve the transition intensity by three times. This method is useful in Doppler laser cooling and detection of macromolecules.


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