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 8
(a, b) Maximum energy exchange, (c, d) form factor peak value and (e, f) form factor frequency at its peak value, calculated as a function of (a, c, e) wiggler gap for E_Laser = 0.4 mJ and (b, d, f) laser pulse energy for a gap of 17 mm. In (c)–(f), (red dots) first turn and (blue dots) second turn. In (c), (black triangles) ratio of first over second-turn form factor maximum intensities. $[\Delta{T_{\rm{Laser}}}]$ = 35 fs FWHM, Z_R = 0.35 m.

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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