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Doppler-Free Comb-Spectroscopy in Counter-Propagating Fields

Received: 26 May 2013    Accepted:     Published: 10 July 2013
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Abstract

The method of Doppler – free comb – spectroscopy for dipole transitions was proposed. The numerical calculations for susceptibility spectrum for two-level system driving by strong counter propagating combs were made. The narrow peaks with homogeneous width arise on the background of Doppler counter. The contrast of these peaks is large for largest amplitudes of comb-components. Power broadening is increasing with increasing of field amplitudes. The amplitudes of peaks depend on the phase difference between carrier frequencies of combs. The spectral range of absorption spectrum is determined by the spectral range of comb generator and all homogeneous lines arise simultaneously. The spectral resolution is determined by the width of homogeneously –broadening lines. The physical nature of narrow peaks is in the existing of multi-photon transitions between manifolds of quasi-energy levels arising for different groups of atoms moving with velocities that satisfy to the resonant conditions 2kv= (n+l)Ω⁄j, where n, l, j-are integers and Ω - frequency difference between comb teeth.

Published in American Journal of Modern Physics (Volume 2, Issue 4)
DOI 10.11648/j.ajmp.20130204.18
Page(s) 223-226
Creative Commons

This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2024. Published by Science Publishing Group

Keywords

Doppler – Free Comb Nonlinear Spectroscopy in Counter – Propagating Comb Laser Fields

References
[1] S.A. Diddams, J.Opt. Soc. Am. B 27, 51 (2010).
[2] A. Schliesser, N. Picque, T.W. Hansch, Nature Photonics 6, 440 (2012).
[3] S. Reinhardt, T. Peters, T.W. Hansch, et.al. Phys. Rev. A 81, 033427 (2010).
[4] E. Peters, S.A. Diddams, P. Fendel, et.al.Optics Express 17, 92 (2009).
[5] S. Stenholm, Foundations of laser spectroscopy (Wiley, New York, 1984; Mir, Moscow, 1987).
[6] T.H. Yoon, S.A. Pulkin, J.R. Park, et.al. Phys. Rev. A 60, 605 (1999).
[7] S.A.Pulkin, T.H. Yoon, A.I. Kuzmin, S.V. Uvarova, Optics and Spectr.105, 288 (2008).
[8] J.H. Shirley, Opt. Letters. 7, 537 (1982).
[9] G.Camy, C.J. Borde, M. Ducloy, Opt. Com. 41, 325 (1982).
[10] V. Arnautov, Master degree thesis, Saint-Petersburg University, Saint-Petersburg, 2012
Cite This Article
  • APA Style

    Sergey A. Pulkin, GuangHoon Kim, Uk Kang, Vasiliy Arnautov, Svetlana V. Uvarova. (2013). Doppler-Free Comb-Spectroscopy in Counter-Propagating Fields. American Journal of Modern Physics, 2(4), 223-226. https://doi.org/10.11648/j.ajmp.20130204.18

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    ACS Style

    Sergey A. Pulkin; GuangHoon Kim; Uk Kang; Vasiliy Arnautov; Svetlana V. Uvarova. Doppler-Free Comb-Spectroscopy in Counter-Propagating Fields. Am. J. Mod. Phys. 2013, 2(4), 223-226. doi: 10.11648/j.ajmp.20130204.18

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    AMA Style

    Sergey A. Pulkin, GuangHoon Kim, Uk Kang, Vasiliy Arnautov, Svetlana V. Uvarova. Doppler-Free Comb-Spectroscopy in Counter-Propagating Fields. Am J Mod Phys. 2013;2(4):223-226. doi: 10.11648/j.ajmp.20130204.18

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  • @article{10.11648/j.ajmp.20130204.18,
      author = {Sergey A. Pulkin and GuangHoon Kim and Uk Kang and Vasiliy Arnautov and Svetlana V. Uvarova},
      title = {Doppler-Free Comb-Spectroscopy in Counter-Propagating Fields},
      journal = {American Journal of Modern Physics},
      volume = {2},
      number = {4},
      pages = {223-226},
      doi = {10.11648/j.ajmp.20130204.18},
      url = {https://doi.org/10.11648/j.ajmp.20130204.18},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajmp.20130204.18},
      abstract = {The method of Doppler – free comb – spectroscopy for dipole transitions was proposed. The numerical calculations for susceptibility spectrum for two-level system driving by strong counter propagating combs were made. The narrow peaks with homogeneous width arise on the background of Doppler counter. The contrast of these peaks is large for largest amplitudes of comb-components. Power broadening is increasing with increasing of field amplitudes. The amplitudes of peaks depend on the phase difference between carrier frequencies of combs. The spectral range of absorption spectrum is determined by the spectral range of comb generator and all homogeneous lines arise simultaneously. The spectral resolution is determined by the width of homogeneously –broadening lines. The physical nature of narrow peaks is in the existing of multi-photon transitions between manifolds of quasi-energy levels arising for different groups of atoms moving with velocities that satisfy to the resonant conditions 2kv= (n+l)Ω⁄j, where n, l, j-are integers and Ω - frequency difference between comb teeth.},
     year = {2013}
    }
    

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  • TY  - JOUR
    T1  - Doppler-Free Comb-Spectroscopy in Counter-Propagating Fields
    AU  - Sergey A. Pulkin
    AU  - GuangHoon Kim
    AU  - Uk Kang
    AU  - Vasiliy Arnautov
    AU  - Svetlana V. Uvarova
    Y1  - 2013/07/10
    PY  - 2013
    N1  - https://doi.org/10.11648/j.ajmp.20130204.18
    DO  - 10.11648/j.ajmp.20130204.18
    T2  - American Journal of Modern Physics
    JF  - American Journal of Modern Physics
    JO  - American Journal of Modern Physics
    SP  - 223
    EP  - 226
    PB  - Science Publishing Group
    SN  - 2326-8891
    UR  - https://doi.org/10.11648/j.ajmp.20130204.18
    AB  - The method of Doppler – free comb – spectroscopy for dipole transitions was proposed. The numerical calculations for susceptibility spectrum for two-level system driving by strong counter propagating combs were made. The narrow peaks with homogeneous width arise on the background of Doppler counter. The contrast of these peaks is large for largest amplitudes of comb-components. Power broadening is increasing with increasing of field amplitudes. The amplitudes of peaks depend on the phase difference between carrier frequencies of combs. The spectral range of absorption spectrum is determined by the spectral range of comb generator and all homogeneous lines arise simultaneously. The spectral resolution is determined by the width of homogeneously –broadening lines. The physical nature of narrow peaks is in the existing of multi-photon transitions between manifolds of quasi-energy levels arising for different groups of atoms moving with velocities that satisfy to the resonant conditions 2kv= (n+l)Ω⁄j, where n, l, j-are integers and Ω - frequency difference between comb teeth.
    VL  - 2
    IS  - 4
    ER  - 

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Author Information
  • Saint-Petersburg State University,Dept.of General Physics 1 of Physical Faculty, Saint-Petersburg, Russia;Russia-Seoul Science, Seoul, Republic of Korea

  • Russia-Seoul Science, Seoul, Republic of Korea

  • Russia-Seoul Science, Seoul, Republic of Korea

  • Saint-Petersburg State University,Dept.of General Physics 1 of Physical Faculty, Saint-Petersburg, Russia

  • Saint-Petersburg State University,Dept.of General Physics 1 of Physical Faculty, Saint-Petersburg, Russia

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