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 5
Exemplary smallest achievable focus spot sizes at both IPs in TMO, obtained from calculations based on start-to-end simulations for LCLS-II with 20 pC bunch charge. The top panel refers to the IP1 (NAMASTE) reaching 2 keV. The bottom panel refers to the IP2 (DREAM) chamber and can reach 1.4 keV.

JOURNAL OF
SYNCHROTRON
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ISSN: 1600-5775

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

https://doi.org/10.1107/S1600577522004283

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