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 9
Ratio of charge state yield versus XGMD pulse energy for 5 fs (blue) and 12 fs (orange) electron bunch duration and at a photon energy of 1050 eV. Pulse energies are measured in the XGMD upstream of the target. The charge states 9+ and 10+ were not observed in the single-shot spectra. The shown ratios are in good agreement with the literature for this photon energy (Young et al., 2010

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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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