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Linac Coherent Light Source II injector commissioning and early operational experience

F. Zhou*, G. Adhikari, A. Brachmann, D. Cesar, W. Colocho, Y. Ding, D. Dowell, G. Just, D. Kennedy et al.

D. Magana, A. Osman, R. Roussel, N. Sudar, T. Vecchione, Z. Zhang, and C. Zimmer

  • *Contact author: zhoufeng@slac.stanford.edu

Phys. Rev. Accel. Beams 29, 104501 – Published 15 October, 2026

DOI: https://doi.org/10.1103/1wk3-p29y

Abstract

The Linac Coherent Light Source II (LCLS-II) is designed to generate 4 GeV electron bunches at an up-to-1-MHz-high repetition rate to drive x-ray free electron lasers. It has been in user operation since 2023 and has progressively ramped up the beam repetition rate to 93 kHz to date. The LCLS-II 1-MeV electron source was successfully commissioned between 2018 and 2020. The full-scale LCLS-II injector, operating above 75 MeV, began commissioning in 2022 and transitioned to operations a few months later. The LCLS-II injector has demonstrated the ability to deliver a high-brightness, low-emittance electron beam at high repetition rates, meeting key performance targets. However, several operational challenges have emerged during commissioning and early user operations. These include substantial gun dark current, the dependence of bunch charge generation and free-electron laser pulse intensity on the beam repetition rate, the formation of cathode quantum efficiency craters and bumps, significant emittance growth through the laser heater chicane, beam breakup, and the presence of beam halos. This paper presents recent progress in addressing these challenges, along with injector emittance measurements and optimizations, and the first demonstration of operating a laser heater undulator at the third-harmonic resonance.

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References (24)

  1. P. Emma et al., First lasing and operation of an angstrom-wavelength free-electron laser, Nature Photon. 4, 641 (2010).
  2. W. Ackermann et al., Operation of a free electron laser in the wavelength range from the extreme ultraviolet to water window, Nature Photon. 1, 336 (2007).
  3. H. Tanaka, Status report on the commissioning of the Japanese XFEL at SPring-8, in Proceedings of IPAC11, San Sebastian, Spain (EPS-AG, Spain, 2011), p. 21.
  4. F. Nolting, C. Bostedt, T. Schietinger, and H. Braun, The Swiss light source and SwissFEL at the Paul Scerrer institute, Eur. Phys. J. Plus 138, 126 (2023).
  5. J. Galayda, LCLS-II: A high power upgrade to the LCLS, in Proceedings of IPAC2018, Vancouver, Canada, p. 18.
  6. J. Schmerge et al., The LCLS-II injector design, in Proceedings of FEL2014, Basel, Switzerland, p. 815.
  7. F. Zhou et al., LCLS-II injector beamline design and RF coupler correction, in Proceedings of FEL 2015, Daejeon, Korea (2015), p. 77.
  8. F. Sannibale et al., Advanced photoinjector experiment photogun commissioning results, Phys. Rev. ST Accel. Beams 15, 103501 (2012).
  9. C. Mitchell et al., RF injector beam dynamics optimization and injected beam energy constraints for LCLS-II, in Proceedings of IPAC2016, Busan, Korea, p. 1699.
  10. R. P. Wells, W. Ghiorso, J. Staples, T. M. Huang, F. Sannibale, and T. D. Kramasz, Mechanical design and fabrication of the VHF-gun, the Berkeley normal-conducting continuous-wave high-brightness electron source, Rev. Sci. Instrum. 87, 023302 (2016).
  11. F. Zhou et al., Commissioning of the SLAC linac coherent light source II electron source, Phys. Rev. Accel. Beams 24, 073073401 (2021).
  12. ASTRA manual, https://www.desy.de/~mpyflo/.
  13. S. Gilevich et al., Report No. SLAC-TN-20-003, 2020.
  14. N. Pandya, Private communication, SLAC (2026).
  15. T. Luo and D. Dowell, Recent new cathode development for LCLS-II photoinjector, AD forum, SLAC (2025).
  16. X.-H. Wang, G. Shu, H.-J. Qian, X.-D. Li, Z.-P. Liu, Z.-G. Jiang, H. Meng, C.-C. Xing, Q. Zhou, and H.-X. Deng, Experimental demonstration of dark current mitigation by an over-inserted plug in a normal conducting very-high-frequency gun, Phys. Rev. Accel. Beams 28, 043401 (2025).
  17. F. Zhou et al., LCLS-II injector operational challenges and recent developments, in Proceeding of NAPAC25, Sacramento, California, USA (2025), pp. 680–682, 10.184229/JACoW-NAPAC2025-WECN01.
  18. M. Gaowei and J. Smedley, Private Communication (2026).
  19. Z. Zhang et al., Beam halo formation via longitudinal-transverse coupling in CW photoinjectors, arXiv:2511.05831.
  20. Z. Zhang, Y. Ding, and F. Zhou, Fault-tolerance analysis for an injector of continuous-wave free-electron lasers, Phys. Rev. Accel. Beams 28, 090701 (2025).
  21. R. Roussel, C. Mayes, A. Edelen, and A. Bartnik, Xopt: A simplified framework for optimization of accelerator problems using advanced algorithms, in Proc. IPAC’23, Venice, Italy (2023), pp. 4847–4850.
  22. R. Roussel et al., Autonomous operation of the DIAG0 diagnostic line for 6D phase-space monitoring at LCLS-II, arXiv:2604.20125.
  23. L. Alsberg et al., LCLS-SC operation status and the LCLS-II-HE upgrade, in Proceeding of SRF2025, Tokyo, Japan (2025), pp. 20–25.
  24. Z. Huang et al., Measurements of the linac coherent light source laser heater and its impact on the x-ray free-electron laser performance, Phys. Rev. ST Accel. Beams 13, 020703 (2010).

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