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Design of Ultrahigh Energy Resolution RIXS Beamline at NanoTerasu
by
Ohtsubo, Yoshiyuki
, Inami, Nobuhito
, Fujii, Kentaro
, Inaba, Kento
, Agui, Akane
, Miyawaki, Jun
, Imazono, Takashi
, Horiba, Koji
, Nakatani, Takeshi
, Kimura, Hiroaki
, Takahasi, Masamitu
in
Dispersion
/ Energy resolution
/ Entrances
/ Optical design
/ Photons
/ Physics
/ Slits
2022
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Design of Ultrahigh Energy Resolution RIXS Beamline at NanoTerasu
by
Ohtsubo, Yoshiyuki
, Inami, Nobuhito
, Fujii, Kentaro
, Inaba, Kento
, Agui, Akane
, Miyawaki, Jun
, Imazono, Takashi
, Horiba, Koji
, Nakatani, Takeshi
, Kimura, Hiroaki
, Takahasi, Masamitu
in
Dispersion
/ Energy resolution
/ Entrances
/ Optical design
/ Photons
/ Physics
/ Slits
2022
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Design of Ultrahigh Energy Resolution RIXS Beamline at NanoTerasu
by
Ohtsubo, Yoshiyuki
, Inami, Nobuhito
, Fujii, Kentaro
, Inaba, Kento
, Agui, Akane
, Miyawaki, Jun
, Imazono, Takashi
, Horiba, Koji
, Nakatani, Takeshi
, Kimura, Hiroaki
, Takahasi, Masamitu
in
Dispersion
/ Energy resolution
/ Entrances
/ Optical design
/ Photons
/ Physics
/ Slits
2022
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Design of Ultrahigh Energy Resolution RIXS Beamline at NanoTerasu
Journal Article
Design of Ultrahigh Energy Resolution RIXS Beamline at NanoTerasu
2022
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Overview
The optical design of the ultrahigh-resolution RIXS beamline, which is currently developed at NanoTerasu in Japan, is described. The main goal of this beamline is to perform ultrahigh-resolution RIXS measurements with a total energy resolution of <10 meV at 250–1000 eV with E /Δ E >150,000 for both beamline and RIXS spectrometer. To achieve the ultra-high resolution, a 2D-RIXS spectrometer using energy-dispersive X-ray is employed to compensate for lower throughput at higher energy resolution, and the optics of the beamline is optimized for the 2D-RIXS spectrometer. A vertically dispersing in-focus variable-included-angle varied-line-spacing plane grating monochromator is employed for the beamline, with an entrance slit to ensure the ultrahigh resolution. First and second mirrors focus X-ray on entrance slits vertically and horizontally, respectively, and the divergent X-ray is irradiated onto the grating. For the 2D-RIXS spectrometer, there is no exit slit, and the vertically energy-dispersed X-ray is irradiated directly onto a sample. In front of the sample, X-ray is horizontally refocused by a Wolter type-I mirror. The expected horizontal focus size at the sample is ~0.7 μm. The expected photon flux is ~1×10 11 photons/s at 500–1000 eV with a virtual slit width of 2 μm required for E /Δ E >150,000. The height of the dispersed X-ray available in the 2D-RIXS spectrometer is ~120 μm, which allows the use of a remarkably high flux of ~6×10 12 photons/s, and the beamline will serve as an ultrahigh-resolution and high-efficiency RIXS facility.
Publisher
IOP Publishing
Subject
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