• Laser & Optoelectronics Progress
  • Vol. 59, Issue 11, 1129001 (2022)
Yingle Li1、*, Mingjun Wang2, and Qunfeng Dong3
Author Affiliations
  • 1College of Information Engineering, Shaanxi Preschool Normal University, Xi'an 710100, Shaanxi , China
  • 2College of Automation and Information Engineering, Xi'an University of Technology, Xi'an 710048, Shaanxi , China
  • 3College of Physics and Electronic Engineering, Xianyang Normal University, Xianyang 712000, Shaanxi , China
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    DOI: 10.3788/LOP202259.1129001 Cite this Article Set citation alerts
    Yingle Li, Mingjun Wang, Qunfeng Dong. Elliptical Gaussian Beam Scattering and Modeling of Finite Length Anisotropic Medium Cylinder[J]. Laser & Optoelectronics Progress, 2022, 59(11): 1129001 Copy Citation Text show less

    Abstract

    In this paper, based on the law of conservation of electromagnetic energy, a model of equating the electromagnetic anisotropic medium to be the electromagnetic isotropic medium is established, and its correctness is verified. Under the condition of the electromagnetic wave length being comparable to the geometrical parameters of the cylinder,the equivalent permittivity of the cylinder of gypsum crystal in the elliptical Gaussian beam varies with its geometrical parameters, beam parameters and beam propagation direction are studied. The simulation results show that the equivalent permittivity fluctuated changes with the increase of the radius of the cylinder, and the change of the equivalent permittivity is very small with the increase of the length of the cylinder. In addition, the analytical expression of the scattered field of an anisotropic cylinder being irradiated by an electromagnetic wave beam with an arbitrary direction is presented. The simulation results show that the radius of the cylinder and the angle between the electromagnetic wave propagation direction and the symmetry axis of the cylinder have a great effect on the scattering, and the length of the cylinder, the distance between the beam and cylinder and the beam waist width etc. have little effects on scattering.
    ε=ε1000ε2000ε3,μ=μ1000μ2000μ3
    -12SE×H*·ds=jω2VBH*-ED*dv
    VμeqH2-εeqE2dv=Vμ1Hx2+μ2Hy2+μ3Hz2-ε1Ex2-ε2Ey2-ε3Ez2dv
    Es,p,ξ=usfs,p,ξ
    us=uxcosθicosφi+cosθisinφiuy-sinθiuzs=cosθicosφix+dsinθicosφi+cosθisinφiy+dsinθisinφi-sinθiz+dcosθip=-sinφix+dsinθicosφi+cosφiy+dsinθisinφiζ=sinθicosφix+dsinθicosφi+sinθisinφiy+dsinθisinφi+cosθiz+dcosθi
    us=ux,s=x,p=y,ξ=z
    Eix,y,z=usE0-QsQpexpjQss2w0s2+jQpp2w0p2exp-jk0ξ
    Qs=1/-j+2ξkw0s2,Qp=1/-j+2ξkw0p2
    us=cos θicosφ-φiuρ-cos θisinφ-φiuφ-sin θiuz
    Eix,y,z=usE0-QsQpexp-jk0dexpjQss2w0s2+jQpp2w0p2exp-jρkρcosφ-φiexp-jβ0z,β0=k0cos θi,kρ=k0sin θi
    Ei=na1nm1nkρ+a2nm2nkρ+b1nn1nkρ+b2nn2nkρ×exp-jβ0zHi=-k0jωμ0na1nn1nkρ+a2nn2nkρ+b1nm1nkρ+b2nm2nkρ×exp-jβ0z
    m1nkρ=-nρJnkρρsinnφuρ-ρJnkρρcosnφuφm2nkρ=nρJnkρρcosnφuρ-ρJnkρρsinnφuφn1nkρ=-jβ0k0ρJnkρρcosnφuρ+jβ0nk0ρJnkρρsinnφuφ+kρ2k0Jnkρρcosnφuzn2nkρ=-jβ0k0ρJnkρρsinnφuρ-jβ0nk0ρJnkρρcosnφuφ+kρ2k0Jnkρρsinnφuz
    a1nSm1nkρm1nkρ×exp-jβ0zds+a2n0+b1n0+b2nSn2nkρm1nkρ×exp-jβ0zds=SEim1n'kρds
    a1n0+a2nSm2nkρm2nkρ×exp-jβ0zds+b1nSn1nkρm2nkρ×exp-jβ0zds+b2n0=SEim2nkρds
    a1n0+a2nSm2nkρn1nkρ×exp-jβ0zds+b1nSn1nkρn1nkρ×exp-jβ0zds+b2n0=SEin1nkρds
    a1nSm1nkρn2nkρ×exp-jβ0zds+a2n0+b1n0+b2nSn2nkρn2nkρ×exp-jβ0zds=SEin2nkρds
    Es=na1nsm1nkρ+a2nsm2nkρ+b1nsn1nkρ+b2nsn2nkρ×exp-jβzHs=-k0jωμ0na1nsn1nkρ+a2nsn2nkρ+b1nsm1nkρ+b2nsm2nkρ×exp-jβz
    Et=na1ntm1nktρ+a2ntm2nktρ+b1ntn1nktρ+b2ntn2nktρ×exp-jβtzHt=-ktjωμ0na1ntn1nktρ+a2ntn2nktρ+b1ntm1nktρ+b2ntm2nktρ×exp-jβtz
    AX=B
    A= 0-ρHn2 jβnk0ρ0Hn200ρJnktρρ0-jβnktρ0Jnktρρ00-ρHn200-jβnk0ρ0Hn2ρJnktρρ000jβnktρ0Jnktρρ0000kρ2k0Hn2000-ktρ2ktJnktρρ000kρ2k0Hn2000-ktρ2ktJnktρρ00jβnρ0Hn200-k0ρHn2 -jβnρ0Jnktρρ000ktρJnktρρ00jβnρ0Hn2k0ρHn200-jβnρ0Jnktρρ0-ktρJnktρρ000kρ2Hn2000-ktρ2Jnktρρ000kρ2Hn2000-ktρ2Jnktρρ0000(1)
    B=a2nρJnkρρ0-b1njβnk0ρ0Jnkρρ0a1nρJnkρρ0+b2njβnk0ρ0Jnkρρ0-b2nkρ2k0Jnkρρ0-b1nkρ2k0Jnkρρ0-a1njβnρ0Jnkρρ0+b2nk0ρJnkρρ0-a2njβnρ0Jnkρρ0-b1nk0ρJnkρρ0-a2nkρ2Jnkρρ0-a1nkρ2Jnkρρ0,(1)
    X=a1nsa2nsb1nsb2nsa1nta2ntb1ntb2ntT=A-1B
    ε=ε1+ε2+ε33,μ=μ1+μ2+μ33
    εeq=Vε1Ex2+ε2Ey2+ε3Ez2dvVE2dv
    Yingle Li, Mingjun Wang, Qunfeng Dong. Elliptical Gaussian Beam Scattering and Modeling of Finite Length Anisotropic Medium Cylinder[J]. Laser & Optoelectronics Progress, 2022, 59(11): 1129001
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