Highly efficient beamline and spectrometer for inelastic soft X-ray scattering at high resolution

Lai, C.H.; Fung, H.S.; Wu, W.B.; Huang, H.Y.; Fu, H.W.; Lin, S.W.; Huang, S.W.; Chiu, C.C.; Wang, D.J.; Huang, L.J.; Tseng, T.C.; Chung, S.C.; Chen, C.T.; Huang, D.J.

doi:10.1107/S1600577513030877

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Figure 4
Simulations of the resolving power of the AGM for the entrance slit widths of 2, 5 and 10 µm and the exit width of 3 µm. The resolving power is defined as $[E/{\Delta}E]$ , where E is the photon energy and ΔE is the energy resolution. All simulations were performed with $[\alpha-\beta]$ = 174°, r₁ = 3.5 m, r₂ = 2.5 m, n₀ = 1200 grooves mm⁻¹, n₁ = 0.8 grooves mm⁻² and slope error = 0.25 µrad r.m.s.

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

Volume 21| Part 2| January 2014| Pages 325-332

doi:10.1107/S1600577513030877

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