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TY - CONF AU - Doolittle, L.R. AU - Babel, S. AU - Bachimanchi, R. AU - Benwell, A.L. AU - Boyes, M. AU - Brown, G.W. AU - Campbell, K.S. AU - Cha, D. AU - Chase, B.E. AU - Cullerton, E. AU - De Long, J.H. AU - Diaz Cruz, J.A. AU - Du, Q. AU - Einstein, J. AU - Greg, D.B. AU - Hong, B. AU - Hovater, C. AU - Huang, G. AU - Jones, J.A. AU - Kelly, R.S. AU - Klepec, D.W. AU - McCollough, A. AU - Ratti, A. AU - Rivetta, C.H. AU - Seidman, D.J. AU - Serrano, C. AU - Vytla, V.K. ED - Schaa, Volker RW ED - He, Yuan ED - Li, Lu ED - Zhao, Ning TI - High Precision RF Control for SRF Cavities in LCLS-II J2 - Proc. of SRF2017, Lanzhou, China, July 17-21, 2017 C1 - Lanzhou, China T2 - International Conference on RF Superconductivity T3 - 18 LA - english AB - The unique properties of SRF cavities enable a new generation of X-ray light sources in XFEL and LCLS-II. The LCLS-II design calls for 280 L-band cavities to be operated in CW mode with a Q_{L} of 4x10⁷, using Single-Source Single-Cavity control. The target RF field stability is 0.01% and 0.01 degree for the band above 1 Hz. Hardware and software implementing a digital LLRF system has been constructed by a four-lab collaboration to minimize known contributors to cavity RF field fluctuation. Efforts include careful attachment to the phase reference line, and minimizing the effects of RF crosstalk by placing forward and reverse signals in chassis separate from the cavity measurement. A low-noise receiver/digitizer section will allow feedback to operate with high proportional gain without excessive noise being sent to the drive amplifier. Test results will show behavior on prototype cryomodules at FNAL and JLab, ahead of the 2018 final accelerator installation. PB - JACoW CP - Geneva, Switzerland SP - 944 EP - 950 KW - ion KW - cavity KW - controls KW - LLRF KW - feedback DA - 2018/01 PY - 2018 SN - 978-3-95450-191-5 DO - 10.18429/JACoW-SRF2017-FRXBA02 UR - http://jacow.org/srf2017/papers/frxba02.pdf ER -