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arXiv 2012.14243physics.plasm-ph
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Characterization of 1- and 2-$μ$m-wavelength laser-produced microdroplet-tin plasma for generating extreme-ultraviolet light

Advanced Research Center for Nanolithography(先进纳米光刻研究中心);Industrial Focus Group XUV Optics, MESA+ Institute for Nanotechnology, University of Twente(特温特大学MESA+纳米技术研究所XUV光学工业聚焦小组);Department of Physics and Astronomy, and LaserLaB, Vrije Universiteit(自由大学物理与天文学系及LaserLaB实验室);Zernike Institute for Advanced Materials, University of Groningen(格罗宁根大学泽尔尼克高级材料研究所)

R. Schupp, L. Behnke, J. Sheil, Z. Bouza, M. Bayraktar, W. Ubachs, R. Hoekstra, O. O. Versolato

英文摘要:

Experimental spectroscopic studies are presented, in a 5.5--25.5nm extreme-ultraviolet (EUV) wavelength range, of the light emitted from plasma produced by the irradiation of tin microdroplets by 5-ns-pulsed, 2-$μ$m-wavelength laser light. Emission spectra are compared to those obtained from plasma driven by 1-$μ$m-wavelength Nd:YAG laser light over a range of laser intensities spanning approximately $0.3-5 \times 10^{11}$Wcm$^{-2}$, under otherwise identical conditions. Over this range of drive laser intensities, we find that similar spectra and underlying plasma charge state distributions are obtained when keeping the ratio of 1-$μ$m to 2-$μ$m laser intensities fixed at a value of 2.1(6), which is in good agreement with RALEF-2D radiation-hydrodynamic simulations. Our experimental findings, supported by the simulations, indicate an approximately inversely proportional scaling $\sim λ^{-1}$ of the relevant plasma electron density, and of the aforementioned required drive laser intensities, with drive laser wavelength $λ$. This scaling also extends to the optical depth that is captured in the observed changes in spectra over a range of droplet diameters spanning 16-51$μ$m at a constant laser intensity that maximizes the emission in a 2\% bandwidth around 13.5nm relative to the total spectral energy, the bandwidth relevant for EUV lithography. The significant improvement of the spectral performance of the 2-$μ$m- vs 1-$μ$m driven plasma provides strong motivation for the development of high-power, high-energy near-infrared lasers to enable the development of more efficient and powerful sources of EUV light.

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