• Chinese Physics B
  • Vol. 29, Issue 9, (2020)
Honggeng Wang1,2, Qiying Song1, Yi Cai1, Qinggang Lin1..., Xiaowei Lu1,†, Huangcheng Shangguan1, Yuexia Ai1 and Shixiang Xu1|Show fewer author(s)
Author Affiliations
  • 1Shenzhen Key Laboratory of Micro-Nano Photonic Information Technology, College of Physics and Optoelectronic Engineering, Shenzhen University, Shenzhen 58060, China
  • 2Key Laboratory of Optoelectronic Devices and Systems and Ministry of Education and Guangdong Province, College of Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, China
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    DOI: 10.1088/1674-1056/aba2df Cite this Article
    Honggeng Wang, Qiying Song, Yi Cai, Qinggang Lin, Xiaowei Lu, Huangcheng Shangguan, Yuexia Ai, Shixiang Xu. Recent advances in generation of terahertz vortex beams and their applications[J]. Chinese Physics B, 2020, 29(9): Copy Citation Text show less

    Abstract

    Last decade has witnessed a rapid development of the generation of terahertz (THz) vortex beams as well as their wide applications, mainly due to their unique combination characteristics of regular THz radiation and orbital angular momentum (OAM). Here we have reviewed the ways to generate THz vortex beams by two representative scenarios, i.e., THz wavefront modulation via specific devices, and direct excitation of the helicity of THz vortex beams. The former is similar to those wavefront engineering devices in the optical and infrared (IR) domain, but just with suitable THz materials, while the latter is newly-developed in THz regime and some of the physical mechanisms still have not been explained explicitly enough though, which would provide both challenges and opportunities for THz vortex beam generation. As for their applications, thanks to the recent development of THz optics and singular optics, THz vortex beams have potentials to open doors towards a myriad of practice applications in many fields. Besides, some representative potential applications are evaluated such as THz wireless communication, THz super-resolution imaging, manipulating chiral matters, accelerating electron bunches, and detecting astrophysical sources.
    1h=lλ/Δn.(1)

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    u(r,θ)=circ(rR)exp(ilθ),(2)

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    \boldsymbolH=(cos2αsin2αsin2αcos2α).(3)

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    Eout=(cos2αsin2αsin2αcos2α)(1001)(1±i)(1000)=exp(±2iα)(10),(4)

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    EQR=[100i]E0(r;ω)[cosLθsinLθ]=E0(r;ω)[cosLθisinLθ],(5)

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    E(r,θ;ω)=22(cosLθ+isinLθ)E0(r;ω)=22E0(r;ω)exp(iLθ).(6)

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    I1+cos[lθk(1+12r2)],(7)

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    lθk(1+12r2)=(n+12)π,(8)

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    \boldsymbolP=(cos2θcosθsinθcosθsinθsin2θ),(9)

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    Eout(r,θ;ω)=(cos2θcosθsinθcosθsinθsin2θ)(1±i)E0(r;ω)=E0(r;ω)exp(±iθ)(cosθsinθ),(10)

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    ϕ(x,y)=lθ2πx/Λ,(11)

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    α(x,y)=ϕ(x,y)/2=lθ/2πx/Λ.(12)

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    \boldsymbolJ(x,y)=R(α)(exp(iΓ/2)00exp(iΓ/2))R(α)=cosζ(1111)isinζ(cos2αsin2αsin2αcos2α).(13)

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    D(x,y)=J(x,y)E(x,y)=cosζ(1±i)isinζexp[±ilθ(x,y)i2πx/Λ](1i).(14)

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    Dn(x,y)=1Λ0ΛD(x,y)exp(i2πx/Λ)dx=cosζδn(1±i)isinζδn±1exp[±ilθ(x,y)](1i),(15)

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    \boldsymbolE=E0(r)[cos(lθ)\boldsymboly^+sin(lθ)\boldsymbolz^],(16)

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    (ExTHzEyTHzEzTHz)=E0(r)(03cos(3φ2lθ)cos(φ2lθ)2cos(φ)3cos(3φ2lθ)+sin(φ2lθ)2sin(φ)),(17)

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    (ExTHzEyTHzEzTHz)=12E0(r)(0sin2(lθ)sin(2lθ))=14E0(r)(01(e2ilθ+e2ilθ)/2(e2iθe2ilθ)/i).(18)

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    EαTHz=EyTHzcosα+iEzTHzsinα=14E0(r)[cosα+(sinαcosα2)e2ilθ(sinα+cosα2)e2ilθ],(19)

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    E±αTHz=122E0(r)(1e2ilθ).(20)

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    Eout=(1ii1)(cosθsinθsinθcosθ)(1000)(ExEy)=eiθ(Ex0)ieiθ(0Ex)oreiθ(Ex0)+ieiθ(0Ex).(21)

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    dATHz(r,ωTHz,z)dziκ[E1(r,ω1,z)][E2(r,ω2,z)]=iκE10(r,ω1,z)E20(r,ω2,z)exp[i(l1l2)θ],(22)

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    E1(r,ω1,z)=E10(r,ω1,z)exp(il1θ),(23)

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    E2(r,ω2,z)=E20(r,ω2,z)exp(il2θ),(24)

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    lTHz=(lOPA1lOPA2)λOPA2λOPA1|λOPA2λOPA1|,(25)

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    nRP=n0+nq=n0+nq0exp(iqz),(26)

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    qS=ωc[(1ωp2ω2)1/21].(27)

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    nSVP=n0+nS=n0+nS0exp(iqSz+ilSθ),(28)

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    nDVP=n0+nD=n0+nD0exp(iqDz+iωDtilDθ),(29)

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    Honggeng Wang, Qiying Song, Yi Cai, Qinggang Lin, Xiaowei Lu, Huangcheng Shangguan, Yuexia Ai, Shixiang Xu. Recent advances in generation of terahertz vortex beams and their applications[J]. Chinese Physics B, 2020, 29(9):
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