Beam-Loss Detection for LCLS-II

Alan Fisher, Christine Clarke, Bryce Jacobson, Ruslan Kadyrov, Evan Rodriguez, Leonid Sapozhnikov, James Welch, Schaa, Volker RW (Ed.), Jansson, Andreas (Ed.), Shea, Thomas (Ed.), Olander, Johan (Ed.)
2019
SLAC is now installing LCLS-II, a superconducting electron linac driven by continuous RF at 1.3 GHz. The 4-GeV, 120-kW beam has a maximum rate of nearly 1 MHz and can be switched pulse-by-pulse to either of two undulators, to generate hard and soft x rays. Two detector types measure beam losses. Point beam-loss monitors (PBLMs) set limits at critical loss points: septa, beam stoppers and dumps, halo collimators, protection collimators (which normally receive no loss), and zones with weak
more » ... ng. PBLMs are generally single-crystal diamond detectors, except at the gun, where a scintillator on a PMT is more sensitive to the low-energy (1 MeV) beam. Long beam-loss monitors (LBLMs) use 200-m lengths of radiation-hard optical fiber, each coupled to a PMT, to capture Cherenkov light from loss showers. LBLMs protect the entire 4-km path from gun to beam dump and locate loss points. In most regions two fibers provide redundancy and view the beam from different angles. Loss signals are integrated with a 500-ms time constant and compared to a threshold; if exceeded, the beam is stopped within 0.2 ms. We report on our extensive tests of the detectors and the front-end signal processing.
doi:10.18429/jacow-ibic2019-tuao02 fatcat:gae7clql7bfbhkhcmaogpns6ei