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 13
(a) Maximum intensity of the bolometer signal averaged over ten shots versus electron beam peak current. Black circles: experiment. Black line: quadratic fit. P_Laser = 0.6 W, $[\Delta{T_{\rm{Laser}}}]$ = 500 fs FWHM ± 100 fs, f# = 4.5, wiggler gap = 17.1 mm. (b) Normalized maximum intensity of the bolometer signal versus wiggler gap. P_Laser = 5.1 W, $[\Delta{T_{\rm{Laser}}}]$ = 35 fs FWHM, f# = 2, I = 5 mA in the single bunch of the hybrid mode of operation.

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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