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Parametric Study of CPT Resonance in Rubidium Vapor Cell for Application in Atomic Clock


Affiliations
1 U.R. Rao Satellite Centre, Indian Space Research Organisation, Bangalore-560 017, India
2 Laboratory for Electro-Optics Systems, Indian Space Research Organisation, Bangalore-560 058, India
3 Bhabha Atomic Research Centre, Mumbai-400 085, India
4 Department of Physics, National Institute of Technology, Warangal, Telangana-506 004, India

The performance of Coherent Population Trapping (CPT) based atomic clocks primarily depends on the characteristics of CPT resonance. We have performed experiments to study and optimize the characteristics of CPT resonance in 87Rb atoms by measuring its contrast and full-width-at-half maximum (FWHM) as function of laser excitation and temperature of atomic vapor cells with different dimensions. A four-level atomic model is used to simulate CPT resonance characteristics along the length of atomic vapor cell. The model incorporates scaling law to understand collision dynamics in cells with different radius for a range of laser excitation intensities and the results are compared with experimental data. The quality figure, calculated from the measured values of FWHM and contrast, decreases with increase in laser intensity and improves in cells with higher dimension (radius). The optimum temperature corresponding to maximum quality figure varies with laser excitation intensity as well as cell dimension. The underlying collision dynamics and density effects that are responsible for the observed resonance characteristics are discussed.
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  • Parametric Study of CPT Resonance in Rubidium Vapor Cell for Application in Atomic Clock

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Authors

Rajaiah Kaitha
U.R. Rao Satellite Centre, Indian Space Research Organisation, Bangalore-560 017, India
Manjula R.
Laboratory for Electro-Optics Systems, Indian Space Research Organisation, Bangalore-560 058, India
Pragya Tiwari
Laboratory for Electro-Optics Systems, Indian Space Research Organisation, Bangalore-560 058, India
Minni J. Kappen
Laboratory for Electro-Optics Systems, Indian Space Research Organisation, Bangalore-560 058, India
Shubhajit Biswas
Laboratory for Electro-Optics Systems, Indian Space Research Organisation, Bangalore-560 058, India
Bijoy Raha
Laboratory for Electro-Optics Systems, Indian Space Research Organisation, Bangalore-560 058, India
Swarupananda Pradhan
Bhabha Atomic Research Centre, Mumbai-400 085, India
Venkatappa Rao T.
Department of Physics, National Institute of Technology, Warangal, Telangana-506 004, India
Umesh S. B.
Laboratory for Electro-Optics Systems, Indian Space Research Organisation, Bangalore-560 058, India
Elumalai S.
Laboratory for Electro-Optics Systems, Indian Space Research Organisation, Bangalore-560 058, India
Kalpana Arvind P.
Laboratory for Electro-Optics Systems, Indian Space Research Organisation, Bangalore-560 058, India
Sriram K. V.
Laboratory for Electro-Optics Systems, Indian Space Research Organisation, Bangalore-560 058, India
Prashanth C. Upadhya
Laboratory for Electro-Optics Systems, Indian Space Research Organisation, Bangalore-560 058, India

Abstract


The performance of Coherent Population Trapping (CPT) based atomic clocks primarily depends on the characteristics of CPT resonance. We have performed experiments to study and optimize the characteristics of CPT resonance in 87Rb atoms by measuring its contrast and full-width-at-half maximum (FWHM) as function of laser excitation and temperature of atomic vapor cells with different dimensions. A four-level atomic model is used to simulate CPT resonance characteristics along the length of atomic vapor cell. The model incorporates scaling law to understand collision dynamics in cells with different radius for a range of laser excitation intensities and the results are compared with experimental data. The quality figure, calculated from the measured values of FWHM and contrast, decreases with increase in laser intensity and improves in cells with higher dimension (radius). The optimum temperature corresponding to maximum quality figure varies with laser excitation intensity as well as cell dimension. The underlying collision dynamics and density effects that are responsible for the observed resonance characteristics are discussed.