The time-resolved atomic, molecular and optical science instrument at the Linac Coherent Light Source

Walter, P.; Osipov, T.; Lin, M.-F.; Cryan, J.; Driver, T.; Kamalov, A.; Marinelli, A.; Robinson, J.; Seaberg, M.H.; Wolf, T.J.A.; Aldrich, J.; Brown, N.; Champenois, E.G.; Cheng, X.; Cocco, D.; Conder, A.; Curiel, I.; Egger, A.; Glownia, J.M.; Heimann, P.; Holmes, M.; Johnson, T.; Lee, L.; Li, X.; Moeller, S.; Morton, D.S.; Ng, M.L.; Ninh, K.; O'Neal, J.T.; Obaid, R.; Pai, A.; Schlotter, W.; Shepard, J.; Shivaram, N.; Stefan, P.; Van, X.; Wang, A.L.; Wang, H.; Yin, J.; Yunus, S.; Fritz, D.; James, J.; Castagna, J.-C.

doi:10.1107/S1600577522004283

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Figure 1
Schematic overview of the new LCLS and NEH layout with both accelerators [LCLS (red) and LCLS-II (blue)]. The LCLS-II X-ray laser is shown alongside the existing LCLS. LCLS uses the last third of SLAC's two-mile-long linear accelerator – a hollow copper structure that operates at room temperature and allows the generation of 120 X-ray pulses per second. For LCLS-II, the first third of the copper accelerator has been replaced with a superconducting one, capable of a repetition rate of up to 1 MHz. Future Far Hall layout changes for LCLS-II HE are not included.

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

Volume 29| Part 4| July 2022| Pages 957-968

https://doi.org/10.1107/S1600577522004283

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