• High Power Laser Science and Engineering
  • Vol. 10, Issue 6, 06000e34 (2022)
Simon Roeder1,2,*, Yannik Zobus1,2, Christian Brabetz1, and Vincent Bagnoud1,2,3
Author Affiliations
  • 1GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
  • 2Technische Universität Darmstadt, Darmstadt, Germany
  • 3Helmholtz-Institut Jena, Jena, Germany
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    DOI: 10.1017/hpl.2022.18 Cite this Article Set citation alerts
    Simon Roeder, Yannik Zobus, Christian Brabetz, Vincent Bagnoud, "How the laser beam size conditions the temporal contrast in pulse stretchers of chirped-pulse amplification lasers," High Power Laser Sci. Eng. 10, 06000e34 (2022) Copy Citation Text show less

    Abstract

    In this work, we propose and verify experimentally a model that describes the concomitant influence of the beam size and optical roughness on the temporal contrast of optical pulses passing through a pulse stretcher in chirped-pulse amplification laser systems. We develop an analytical model that is capable of predicting the rising edge caused by the reflection from an optical element in a pulse stretcher, based on the power spectral density of the surface and the spatial beam profile on the surface. In an experimental campaign, we characterize the temporal contrast of a laser pulse that passed through either a folded or an unfolded stretcher design and compare these results with the analytical model. By varying the beam size for both setups, we verify that optical elements in the near- and the far-field act opposed to each with respect to the temporal contrast and that the rising edge caused by a surface benefits from a larger spatial beam size on that surface.
    E(ω)=E0(ω)eiδϕ(ω), ((1))

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    δϕ(ω)=(4π/λ0)H(ω), ((2))

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    E(ω)=f[xaωω]eiδϕ(x)dxE0(ω). ((3))

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    E(ω)=f(xaωω)[1+iδϕ(x)]dxE0(ω), ((4))

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    =E0(ω)+if(xaωω)δϕ(x)dxE0(ω), ((5))

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    E~(t)=E~0(t)+i[eiωtf(xaωω)δϕ(x)dωdx]E~0(t), ((6))

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    E~(t)=E~0(t)+[eixaωtf(x)dxaωeixaωtδϕ(x)dx]E~0(t). ((7))

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    E(t)=E~0(t)iaω[f~(t/aω)δ~ϕ(t/aω)]E~0(t). ((8))

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    I(t)=I0(t)+1aω2|[f~(t/aω)δ~ϕ(t/aω)]E~0(t)|2 ()

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    2aωIm{E~0(t){[f~(t/aω)δ~ϕ(t/aω)]E~0(t)}}. ((9))

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    I(t)=I0(t)+1aω2|[f~(t/aω)δ~ϕ(t/aω)]E~0(t)|2. ((10))

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    I(t)=I0(t)+εsaω2|f~(t/aω)δ~ϕ(t/aω)|2, ((11))

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    PSD=|H~(t/aω)|2Δk, ((12))

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    I(t)=I0(t)+16π2εsaω2λ02Δk|f~(t/aω)|2PSD(t/aω). ((13))

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    Simon Roeder, Yannik Zobus, Christian Brabetz, Vincent Bagnoud, "How the laser beam size conditions the temporal contrast in pulse stretchers of chirped-pulse amplification lasers," High Power Laser Sci. Eng. 10, 06000e34 (2022)
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