Commissioning of a multi-beamline femtoslicing facility at SOLEIL

Labat, M.; Brubach, J.-B.; Ciavardini, A.; Couprie, M.-E.; Elkaim, E.; Fertey, P.; Ferte, T.; Hollander, P.; Hubert, N.; Jal, E.; Laulhé, C.; Luning, J.; Marcouillé, O.; Moreno, T.; Morin, P.; Polack, F.; Prigent, P.; Ravy, S.; Ricaud, J.-P.; Roy, P.; Silly, M.; Sirotti, F.; Taleb, A.; Tordeux, M.-A.; Nadji, A.

doi:10.1107/S1600577518000863

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Figure 9
(i) Spectral intensity of the (a) spectrometer (with turn 2 × 100) and (b) bolometer, calculated for E_L = 0.4 mJ and gap = 17 mm. (ii) Spectrometer and (iii) bolometer maximum intensity and frequency of maximum intensity versus wiggler gap calculated for E_L = 0.4 mJ and versus E_L for gap = 17 mm. In all plots, red lines or dots represent the first, blue the second and green for the third turn. In (ii-a) and (ii-b), second-turn intensity × 100. In (iii-a) and (iii-b), black triangles represent the ratio first over second-turn form factor maximum intensities. Z_R = 0.35 m and $[\Delta{T}]$ = 35 fs FWHM.

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

Volume 25| Part 2| March 2018| Pages 385-398

https://doi.org/10.1107/S1600577518000863

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