• Advanced Photonics Nexus
  • Vol. 2, Issue 3, 036001 (2023)
Jiawei Yan* and Gianluca Geloni*
Author Affiliations
  • European XFEL, Schenefeld, Germany
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    DOI: 10.1117/1.APN.2.3.036001 Cite this Article Set citation alerts
    Jiawei Yan, Gianluca Geloni. Self-seeded free-electron lasers with orbital angular momentum[J]. Advanced Photonics Nexus, 2023, 2(3): 036001 Copy Citation Text show less

    Abstract

    X-ray beams carrying orbital angular momentum (OAM) are an emerging tool for probing matter. Optical elements, such as spiral phase plates and zone plates, have been widely used to generate OAM light. However, due to the high impinging intensities, these optics are challenging to use at X-ray free-electron lasers (XFELs). Here, we propose a self-seeded free-electron laser (FEL) method to produce intense X-ray vortices. Unlike passive filtering after amplification, an optical element will be used to introduce the helical phase to the radiation pulse in the linear regime, significantly reducing thermal load on the optical element. The generated OAM pulse is then used as a seed and significantly amplified. Theoretical analysis and numerical simulations demonstrate that the power of the OAM seed pulse can be amplified by more than two orders of magnitude, reaching peak powers of several tens of gigawatts. The proposed method paves the way for high-power and high-repetition-rate OAM pulses of XFEL light.
    E˜(z,r,ϕ)=n=E˜(n)(z,r)exp(inϕ),

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    E˜(n)(z^,r^)=jaj(n)Φnj(r^)exp(λj(n)z^),

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    [Δn+g(r^,λj(n))]Φnj(r^)+2iBλj(n)Φnj(r^)=0,

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    Δn[2r^2+1r^r^n2r^2],

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    [2+2iωcz]E˜=0,

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    [Δn+2iBz^]Φnj(r^,z^)=0.

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    [Δnl+2iBz^]Φnl,j(Ic)(r^,z^)=0.

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    Φnl,j(Ic)(r^,δz^)=iB2πδz^0dr^r^02πdδϕexp{iB2δz^[r^22r^r^cos(δϕ)+r^2]}×Φnj(I)(r^)exp[i(nl)δϕ].

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    Φnl,j(Ic)(r^,δz^)=inl+1Bδz^exp(iBr^22δz^)0dr^r^exp(iBr^22δz^)Φnj(I)(r^)Jnl(r^r^Bδz^).

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    E˜(r^,ϕ)=n=jaj(n)exp(λj(n)z^1)Φnl,j(Ic)(r^)exp[i(nl)ϕ],

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    E˜(r^,ϕ)=n=a1(n)exp(λ1(n)z^1)Φnl,1(Ic)(r^)exp[i(nl)ϕ]n=A(n)Φnl,1(Ic)(r^)exp[i(nl)ϕ].

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    [Δm+g(r^,λk(II,m))]Φm,k(II)(r^)+2iBλk(II,m)Φm,k(II)(r^)=0,

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    Φnl,1(Ic)(r^,δz^)=kαkΦnl,k(II).

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    E˜(nl)(r^,ϕ)=A(n)kαkΦnl,k(II)exp[i(nl)ϕ]exp(λk(II,nl)z^2),

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    Jiawei Yan, Gianluca Geloni. Self-seeded free-electron lasers with orbital angular momentum[J]. Advanced Photonics Nexus, 2023, 2(3): 036001
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