Development of a multi-functional chamber for resonant X-ray scattering experiments in the tender X-ray regime at the PAL-XFEL

Park, S.H.; Kim, S.; Park, J.; Yun, S.; Jeong, J.; Park, J.-G.; Kim, K.S.; Choi, T.-K.; Eom, I.; Jang, D.; Kim, M.; Lee, J.H.; Park, S.-Y.; Kim, H.; Chun, S.H.

doi:10.1107/S1600577525002899

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Figure 5
(a) X-ray photon energy dependence of the (010) ATS reflection of Li₂RuO₃ across the Ru L₃-edge. (b) Transient intensity changes of the (010) ATS reflection at E_i = 2.841 keV. The optical laser was set to a wavelength of 800 nm with p-polarization, and the X-ray beam had π-polarization within the X-ray scattering plane. (c) Calculated temporal broadening effect as a function of θ_Sample, resulting from the 10° incident angle difference between the pump and probe beams. The pink and cyan curves represent results for X-ray beam size diameters of 200 µm and 20 µm (FWHM), respectively.

JOURNAL OF
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RADIATION

ISSN: 1600-5775

Volume 32| Part 3| May 2025|

https://doi.org/10.1107/S1600577525002899

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