• Chinese Optics Letters
  • Vol. 21, Issue 7, 071901 (2023)
Fanglun Yang1、2、3, Guowen Zhang2、3、4、*, Xiaoqi Zhang2、3, Yanli Zhang2、3, Ruifeng Wang2、3、4, and Jianqiang Zhu2、3、**
Author Affiliations
  • 1School of Physical Sciences, University of Science and Technology of China, Hefei 230026, China
  • 2Key Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 3National Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 4University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.3788/COL202321.071901 Cite this Article Set citation alerts
    Fanglun Yang, Guowen Zhang, Xiaoqi Zhang, Yanli Zhang, Ruifeng Wang, Jianqiang Zhu. Self-focusing of partially coherent beams based on complex screen and split-step Fourier transform methods[J]. Chinese Optics Letters, 2023, 21(7): 071901 Copy Citation Text show less

    Abstract

    The self-focusing phenomenon of partially coherent beams (PCBs) was simulated using the complex screen method combined with the split-step Fourier method to solve the nonlinear Schrödinger equation. Considering the propagation of Gaussian Schell-model beams in a nonlinear medium as an example, the suppression effects of intensity, propagation distance, and spatial coherence on small-scale self-focusing were demonstrated. Simulations of overall and small-scale self-focusing using this method were compared with the existing literature to demonstrate the validity of the method. This method can numerically analyze the degree of self-focusing in PCBs and advance the study of their nonlinearity.
    W(r1,r2,z)=T(r1,z)T*(r2,z)=E(r1)E*(r2)µ(r1,r2).

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    Tn(r)=E(r)ψn(r).

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    W(r1,r2,z)=E(r1)E*(r2)ψn(r1)ψn*(r2).

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    µ(r1,r2)=p(v)exp[i(r1r2)v]dv,

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    Cn(υ1)Cn*(υ2)=δ(υ1υ2),

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    ψn(r)=p(v)Cn(υ)exp(i2πr·v)dv.

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    W(r1,r2,z)1Nn=1NTn(r1)Tn*(r2).

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    W(r1,r2,z)=I0exp(r12+r22ω02)exp[(r1r2)22ρ02],

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    E(r)=E0exp(r2ω02),

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    µ(r1,r2)=W(r1,r2,z)W(r1,r1,z)W(r2,r2,z)=exp[(r1r2)22ρ02],

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    I(r)=|T(r)|21N1N|Tn(r)|2.

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    [2ikz+(1222)]W(r1,r2,z)+2k2n2[W(r1,r1,z)W(r2,r2,z)]n0W(r1,r2,z)=0,

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    2ikzW(r1,r2,z)+(1222)W(r1,r2,z)=0.

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    zW(r1,r2,z)=W(r1,r2,z)×ikn2[W(r1,r1,z)W(r2,r2,z)]n0.

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    W(r1,r2,z+Δz)=W(r1,r2,z)×exp[ikn2[W(r1,r1,z)W(r2,r2,z)]n0×Δz].

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    zTn(r,z)=ikn2|T(r)|2n0Tn(r,z).

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    Tn(r,z+Δz)=exp[ikn2|T(r)|2n0×Δz]×Tn(r,z).

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    t(x,y)=[1+a×sin(2πfxx)]1/2,

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    M=ImaxIminImax+Imin.

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    Fanglun Yang, Guowen Zhang, Xiaoqi Zhang, Yanli Zhang, Ruifeng Wang, Jianqiang Zhu. Self-focusing of partially coherent beams based on complex screen and split-step Fourier transform methods[J]. Chinese Optics Letters, 2023, 21(7): 071901
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