• Photonics Insights
  • Vol. 2, Issue 3, R07 (2023)
Dongdong Zhang1, Yushan Zeng1, Ye Tian1、*, and Ruxin Li1、2、*
Author Affiliations
  • 1State Key Laboratory of High Field Laser Physics and CAS Center for Excellence in Ultra-intense Laser Science, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, China
  • 2School of Physical Science and Technology, ShanghaiTech University, Shanghai, China
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    DOI: 10.3788/PI.2023.R07 Cite this Article Set citation alerts
    Dongdong Zhang, Yushan Zeng, Ye Tian, Ruxin Li. Coherent free-electron light sources[J]. Photonics Insights, 2023, 2(3): R07 Copy Citation Text show less

    Abstract

    Free-electron light sources feature extraordinary luminosity, directionality, and coherence, which has enabled significant scientific progress in fields including physics, chemistry, and biology. The next generation of light sources has aimed at compact radiation sources driven by free electrons, with the advantages of reduction in both space and cost. With the rapid development of ultra-intense and ultrashort lasers, great effort has been devoted to the quest for compact free-electron lasers (FELs). This review focuses on the current efforts and advancements in the development of compact FELs, with a particular emphasis on two notable paths: the development of compact accelerators and the construction of micro undulators based on innovative materials/structures or optical modulation of electrons. In addition, the physical essence of inverse Compton scattering is discussed, which offers remarkable capability to develop an optical undulator with a spatial period that matches the optical wavelength. Recent scientific developments and future directions for miniaturized and integrated free-electron coherent light sources are also reviewed. In the future, the prospect of generating ultrashort electron pulses will provide fascinating means of producing superradiant radiation, promising high brilliance and coherence even on a micro scale using optical micro undulators.

    Story Video to the Review Article

    E2p2c2=me2c4.

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    ω2k2c2=0,

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    ω2k2c2=0,

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    PfPi=Pph+mℏ︀ku,

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    Ei+ℏ︀ω1=Ef+ℏ︀ω2,

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    Piℏ︀ω1/c=Pf+ℏ︀ω2/c.

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    ρ(r,t)=eδ(rre(t)),

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    J(r,t)=eveδ(rre(t)),

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    ρ(r,ω)=eδ(r)exp(iωr/v),

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    J(r,ω)=er^δ(r)exp(iωr/v).

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    E(r,t)=e4πɛ0((1β2)(nβ)k3(rre(t))+n×(nβ)×β˙ck3(rre(t))),

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    B(r,t)=nc×E(r,t).

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    P=23e2mec3(dpdt·dpdt),

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    P=23e2mec3(dpμdτ·dpμdτ),

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    dpμdτ·dpμdτ=(dpdτ)21c2(dEdτ)2=(dpdτ)2β2(dpdτ)2.

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    P=23e2cγ6((β˙)2(β×β˙)2),

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    d2UdωdΩ=e24π2c×|+dteiω(tn·r(t)/c)n×[(nβ)×β˙](1β·n)2|2.

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    2Nxλ=2παλ2(11/β2n2).

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    dEdωdz=z2e2c2ω(11β2ε(ω))H(z)(βn1),

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    dUdωdΩ=μ0e2β2c4π3sin2θ(1βcosθ)2.

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    d2UdΩdω=e216π3ε0cγ2(ωωc)2(1+γ2θ2)2(K3/22(ξ)+γ2θ21+γ2θ2K1/32(ξ)).

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    x(z)=x0sin(kuz)=ψkusin(kuz)=Kγkusin(kuz),

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    βzβ(1K22γ2cos2(kuz)),

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    β¯zβ(1K24γ2)=112γ2(1+K22).

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    mλ=λuβz¯λucosθλu2γ2(1+K22+γ2θ2).

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    λλu2mγ2(1+K22),

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    B6D=Iεnxεny0.1%ΔWW,

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    ω=ωqβn(ωq)cosθq11βcosθ.

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    ω=ωqβn(ωq)cosθq11βcosθ2ωqγ2(βn(ωq)cosθq1),

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    E=meωpca0/e,

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    rb=(2/kp)a0,

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    λu=2γλp,

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    K=γβkpγ/2.

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    B=photons/second(mrad)2(mm2source area)(0.1%band width).

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    EH=2γe2f(a0)1+cosθL1+(γeθγ)+a02+4γeELmec2EL,

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    λγλL4γe21f(a0)(1+a022).

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    λu=βλL1+βλL2.

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    Bu=B+Eβc=(1+β)Bβ2B.

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    λγλu=kukγ=1+(1+β)K2/4+β(1+β)γ2θL2/2β(1+β)γ2.

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    λu=λL/22γ21f(a0)(1+a022),

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    P=|j=1NeA(r,t)exp(iωt+ϕj)|2=|A(r,t)|2(j=1NeNe+|j=1Nek=1Neexp(i(ωtj+ωtk+ϕjϕk))|2),

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    2σtb<T=2π/ω,

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    P=ɛ0E2Σve=12η2Ip2Z0f2βz2Σ,

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    ΔW=eλ2meπcW0Emax,

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    FP=Up=e24meω2EL(r,t)2,

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    UP2EL(t,t0,z,z0)e2me(ω1+ω2)2·cos((ω1ω2)(tt0)(ω1cosαω2cosβ)zz0c+(ϕ1ϕ2)),

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    Dongdong Zhang, Yushan Zeng, Ye Tian, Ruxin Li. Coherent free-electron light sources[J]. Photonics Insights, 2023, 2(3): R07
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