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Volume 27 Issue 2
Sep.  2013
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Article Navigation >  LASER TECHNOLOGY  > 2003 >  27(2): 126-129

Citation:
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Propagation properties of three-dimensional TEMm,n-mode Hermite-Gaussian beams through an optical symmetric system

  • 1.

    Department of Applied Physics, Southwest Jiaotong University, Chengdu, 610031;

  • 2.

    Institute of Laser Physics & Chemistry, Sichuan University, Chengdu, 610064

  • Received Date: 2001-12-18
  • By using the second order moments method and generalized Huygens-Fresnel diffraction integral,the transformation properties of a three-dimensional TEMm,n-mode Hermite-Gaussian beam passing th rough an optical symmetrizing system are studied in detail. It is shown that the symmetrization is complete,because,not only the symmetrizing transformation is achieved in the second order moments sense,but also the output beam becomes a circular one,and then retains its shape unchanged upon propagation.
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    Laabs H,Gao C.J Mod Opt,1999,46(4):709～719.
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    Eppich B,Fiberg A T.SPIE,1996,2870:260～267.
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    Gao C,Laabs H.Opt Quant Electron,1999,34:1207～1218.
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    Gao C.Characterization and transformation of astigmatic laserbeams.Berlin:Wissenschaft und Technik Verlag,1999:19～52.
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    Tamm C,Weiss C O.J O S A,1990,B7:1034～1038.
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    Collins S A.J O S A,1970,A1:1168～1177.
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  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

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Propagation properties of three-dimensional TEMm,n-mode Hermite-Gaussian beams through an optical symmetric system

  • 1. Department of Applied Physics, Southwest Jiaotong University, Chengdu, 610031;
  • 2. Institute of Laser Physics & Chemistry, Sichuan University, Chengdu, 610064
  • Received Date: 2001-12-18
  • Available Online: 2003-03-25

Abstract: By using the second order moments method and generalized Huygens-Fresnel diffraction integral,the transformation properties of a three-dimensional TEMm,n-mode Hermite-Gaussian beam passing th rough an optical symmetrizing system are studied in detail. It is shown that the symmetrization is complete,because,not only the symmetrizing transformation is achieved in the second order moments sense,but also the output beam becomes a circular one,and then retains its shape unchanged upon propagation.

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