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Observe the spontaneous radiation spectrum of individual undulators and FEL radiation with a spectrograph optimized for 800-8000 eV photon energy range. Achieve a spectral resolution of <1x10-3 and a spectral window of >1x10-2. Consider damage from FEL radiation.
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A Grating Spectrograph for the LCLS Philip Heimann Advanced Light Source • Observe the spontaneous radiation spectrum of the individual undulators • Observe the spectrum of FEL radiation
Design criteria • Goals • Photon energy range: 800 – 8000 eV. • Spectral resolution: Dl/l < 1 x 10-3 set by the FEL radiation bandwidth • Spectral window Dl/l > 1 x 10-2 set by the single undulator harmonic energy width • Single shot sensitivity for single undulator spectra. • Consider damage for FEL radiation
Individual undulator spectrum • From Steve Hulbert • We would like to display ~800 eV energy window. • The energy resolution requirement is modest < 60 eV.
Can we use gratings from 800 – 8000 eV? • Heimann, Koike and Padmore Rev. Sci. Instrum. 76, 63102 (2005) • Shimadzu grating: 600 l/mm, laminar, h = 6.5 nm, Au coating, 2.4 A rms • Peak efficiency 14 % • Measured with Surface Normal Rotation (SNR) of 0o and 60o, equivalent to changing d
LCLS grating spectrometer layout • One VLS grating in -1 order • Length of spectrometer 1.3 m
Raytracing of the grating spectrometer: 800 eV 799.2 eV 800 eV 800.8 eV • Source 130 mm diameter (fwhm) 799.2, 800, 800.8 eV or 760, 800, 840 eV • At the detector 3.5 mm (h) x 4 mm (v) (fwhm) DE = 0.4 eV (2 x103 RP, limited by detector pixel size 13 mm) 760 eV 800 eV 840 eV 3 mm
Raytracing of the grating spectrometer: 8000 eV 7992 eV 8000eV 8008 eV • At the detector 1.1 mm (h) x 2 mm (v) (fwhm) DE = 14 eV (6x102 RP , limited by detector pixel size 13 mm, in FEL case could use inclined detector) • Source 90 mm diameter (fwhm) 7992, 8000, 8008 eV or 7600, 8000, 8400 eV 7600 eV 8000 eV 8400 eV 800 mm
Is there single shot sensitivity for spontaneous radiation? • Undulator (1) • Flux F = 1.4 x 1014 N Qn I = 3 x 106 1/(pulse 0.1% bw) • Bandwidth DE/E = 1/N = 8.8 x10-3 • Divergence sr‘ = l/2L = 15 mrad (800 eV) and 4.8 mrad (8 keV) • Spectrometer • Vertical angular acceptance 60 mrad (800 eV) and 20 mrad (8 keV) • Efficiency e = RM1.eG = 0.13 (800 eV) and 0.08 (8000 eV) • Flux at detector 2 - 4 x 105, N noise ~ 0.2 % Yes
Beam damage with LCLS FEL radiation • M1 mirror preliminary estimate: mirror would be OK at 800 eV (0.2 eV/atom) but not at 8 keV (10 eV/atom). • Detector: focusing in one dimension, silicon at normal incidence, would damage at 800 eV (12 eV/atom) and at 8 keV (1.5 eV/atom). • It would be possible to attenuate the FEL beam, e.g. with the gas filter.
Grating beam splitter for spectrometer as a passive diagnostic • Optimize grating efficiency for 0 order, “bad” grating • Parameters: 800 eV, 50 l/mm, q = 89.5o, h = 4 nm, Pt coating (damage?) • E0 = 0.88, E1 = 0.005
Summary: the Grating Spectrograph for the LCLS • Photon energy range: 800 – 8000 eV. • Resolving power: E/DE = 2000 at 800 eV and 600 at 8 keV. • For FEL radiation the resolution could be improved with an inclined detector. • Spectral window: DE/E = 10%. • Single shot sensitivity for single undulator spectra.