• Photonics Research
  • Vol. 9, Issue 5, 803 (2021)
Junli Qi1、2、3、4, Weihua Wang1、2、5、6、*, Bo Shi4, Hui Zhang4, Yanan Shen4, Haifei Deng4, Wenjing Pu4, Xin Liu4, Huihui Shan4, Xiaomin Ma4, Lianqiang Zhang4, Wei Lu5, Meicheng Fu3, and Xiujian Li3、7、*
Author Affiliations
  • 1Institute of Plasma Physics, Hefei Institutes of Physical Sciences, Chinese Academy of Sciences, Hefei 230031, China
  • 2Science Island Branch of Graduate School, University of Science and Technology of China, Hefei 230031, China
  • 3College of Liberal Arts and Sciences, National University of Defense Technology, Changsha 410073, China
  • 4Institute of Applied Physics, Army Academy of Artillery and Air Defense, Hefei 230031, China
  • 5Institute of Physical Science and Information Technology, Anhui University, Hefei 230031, China
  • 6e-mail: whwang@ipp.ac.cn
  • 7e-mail: xjli@nudt.edu.cn
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    DOI: 10.1364/PRJ.419561 Cite this Article Set citation alerts
    Junli Qi, Weihua Wang, Bo Shi, Hui Zhang, Yanan Shen, Haifei Deng, Wenjing Pu, Xin Liu, Huihui Shan, Xiaomin Ma, Lianqiang Zhang, Wei Lu, Meicheng Fu, Xiujian Li. Concise and efficient direct-view generation of arbitrary cylindrical vector beams by a vortex half-wave plate[J]. Photonics Research, 2021, 9(5): 803 Copy Citation Text show less

    Abstract

    A concise, efficient, and practical direct-view scheme is presented to generate arbitrary cylindrical vector (CV) beams, including CV beams, vortex beams, and cylindrical vector vortex (CVV) beams, by a vortex half-wave plate (VHP). Six kinds of first-order and other high-order CV beams, such as azimuthally polarized (AP) beams, antivortex radial polarization mode beams, and three-order AP beams, are formed by simply rotating a half-wave plate. The Stokes parameters and double-slit interference of multitype CV beams are investigated in detail. The polarization parameters, including degree of polarization, polarization azimuth, and ellipticity, are obtained, which demonstrates the efficient generation of CV beams. In addition, the double-slit interference experiment is introduced in the setup, and fringe misplacement and tilt appear for CVV beams, in which the misplacement number M is 2P+1 for P2 and 2P-1 for P3, where P is the polarization order number, and the fringe tilt offset is positively related to the topological charge number l of CVV beams. In addition, new types of VHPs can be formed by cascading two or more VHPs when the types of available VHPs are limited, assisting in more flexible generation of multitype CV beams. It is experimentally demonstrated that arbitrary CV beams with high quality are effectively achieved by the proposed setup, and the double-slit interference method can be utilized to determine and analyze CV beams rapidly and concisely by practical performance, which shows the potential to be implemented as a commercial device.
    θ=m2ψ+σ,

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    Jm,σ=[cos2θsin2θsin2θcos2θ]=[cos(mψ+2σ)sin(mψ+2σ)sin(mψ+2σ)cos(mψ+2σ)],

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    m2ΦΦ=ϕΦ=2ϕm2.

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    ERP=J1,0·E//=[cosψsinψsinψcosψ]·[10]=[cosψsinψ],

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    EAP=J1,π/4·E//=[cos(ψ+π/2)sin(ψ+π/2)]=[sinψcosψ],

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    EAP=J1,0·E=[sinψcosψ]=[cos(ψπ/2)sin(ψπ/2)]=eiπ·EAP,

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    Eπ/41=J1,π/8·E//=[cos(ψ+π/4)sin(ψ+π/4)].

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    Eπ/41=J1,π/8·E//=[cos(ψπ/4)sin(ψπ/4)]=eiπ·[cos(ψ+3π/4)sin(ψ+3π/4)]=eiπ·J1,3π/8·E//.

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    Eαm=Jm,0·Eα=[cos(mψ)sin(mψ)sin(mψ)cos(mψ)]·[cosαsinα]=[cos(mψα)sin(mψα)].

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    EARP=J0·ERP=[1001]·[cosψsinψ]=[cos(ψ)sin(ψ)].

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    EAAP=J0·EAP=Jπ/4·ERP=[0110]·[cosψsinψ]=[sinψcosψ]=[cos(ψ+π/2)sin(ψ+π/2)].

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    Jθ(λ/4)=22[1icos2θisin2θisin2θ1+icos2θ].

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    Jm,σ·EL=22[cos2θ+isin2θsin2θicos2θ]=22[ei2θei(2θπ/2)]=22[1i]·ei(mψ+2σ)=ER·ei(mψ+2σ)=EARCV,

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    Jm,σ·ER=22[cos2θisin2θsin2θ+icos2θ]=22[ei(2θ)ei(2θ+π/2)]=22[1i]·ei(mψ+2σ)=EL·ei(mψ+2σ)=ECLCV,

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    Jπ/4(λ/4)·EARCV=[0i]·ei(mϕ+2σ)=E·ei(mψ+2σπ/2)=EAVLV,Jπ/4(λ/4)·EARCV=[10]·ei(mϕ+2σ)=E//·ei(mψ+2σ)=EAHLV.

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    Jπ/4(λ/4)·ECLCV=[10]·ei(mϕ+2σ)=E//·ei(mψ+2σ)=ECHLV,Jπ/4(λ/4)·ECLCV=[0i]·ei(mϕ+2σ)=E·ei(mψ+2σπ/2)=ECVLV.

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    Jm2,σ2·EAHLV=[cos(m2ψ+2σ2)sin(m2ψ+2σ2)]·ei(m1ψ+2σ1)=ERm2Vm1,Jm2,σ2·EAVLV=[sin(m2ψ+2σ2)cos(m2ψ+2σ2)]·ei(m1ψ+2σ1π/2)=EAm2Vm1.

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    Jm2,σ2·ECHLV=[cos(m2ψ+2σ2)sin(m2ψ+2σ2)]·ei(m1ψ+2σ1)=ERm2Vm1,Jm2,σ2·ECVLV=[sin(m2ψ+2σ2)cos(m2ψ+2σ2)]·ei(m1ψ+2σ1π/2)=EAm2Vm1.

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    J2·J1=Jm2,σ2·Jm1,σ1=[cosα2sinα2sinα2cosα2]·[cosα1sinα1sinα1cosα1]=[cos[(m2m1)ψ+2(σ2σ1)]sin[(m2m1)ψ+2(σ2σ1)]sin[(m2m1)ψ+2(σ2σ1)]cos[(m2m1)ψ+2(σ2σ1)]],

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    (J2·J1)·J0=[cos(α2α1)sin(α2α1)sin(α2α1)cos(α2α1)]·[cos0sin0sin0cos0]=[cos(α2α1+0)sin(α2α1+0)sin(α2α1+0)cos(α2α1+0)].

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    J3·(J2·J1)=[cos(α3α2+α1)sin(α3α2+α1)sin(α3α2+α1)cos(α3α2+α1)].

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    {S0=Ix+Iy=Iπ/4+Iπ/4=IR+IL=I0S1=IxIy=S02Iy=2IxS0S2=Iπ/4Iπ/4=S02Iπ/4=2Iπ/4S0S3=IRIL=S02IL=2IRS0,

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    {p=S12+S22+S32S0ψ=12arctan(S2/S1)χ=12arcsinS3S12+S22+S32,

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    {l=Ri/R1,l>0l=Ri/|R1|,l<0.

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    Junli Qi, Weihua Wang, Bo Shi, Hui Zhang, Yanan Shen, Haifei Deng, Wenjing Pu, Xin Liu, Huihui Shan, Xiaomin Ma, Lianqiang Zhang, Wei Lu, Meicheng Fu, Xiujian Li. Concise and efficient direct-view generation of arbitrary cylindrical vector beams by a vortex half-wave plate[J]. Photonics Research, 2021, 9(5): 803
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