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

Journal of Synchrotron Radiation Journal of
Synchrotron Radiation

IUCr IT WDC

home archive editors for authors for readers submit open access

view article

Figure 3
Overview of the TMO instrument layout, showing both endstations which are capable of taking full advantage of both the high per-pulse energy from the copper accelerator (120 Hz) as well as high average intensity and high repetition rate from the superconducting accelerator (1 MHz). Indicated are the beam-position monitors IM3K4, IM4K4, IM5K4, IM6K4; differential pumping sections PA1K4 and PA2K4; IP1 optical laser in-coupling LI1K4, LI2K4, and IP1 laser out-coupling LI3K4; the arrival-time monitors TM1K4 and TM2K4; wavefront sensor PF1K4 and PF2K4; retractable beam terminators SF1K4 and SF2K4; beamline collimators PC5K4; as well as the interaction points IP1 and IP2; and finally the beam terminator SF3K4.

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

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

https://doi.org/10.1107/S1600577522004283

Open

access

Follow J. Synchrotron Rad.

Search IUCr Journals		doi		Advanced search
Author		volume	page