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TY - CONF AU - Papaevangelou, T. AU - Alves, H. AU - Aune, S. AU - Beltramelli, J. AU - Bertrand, Q. AU - Bey, T. AU - Bolzon, B. AU - Chauvin, N. AU - Combet, M. AU - Desforge, D. AU - Desmons, M. AU - Dolenc Kittelmann, I. AU - Gauthier, Y. AU - Giner-Demange, E. AU - Gomes, A. AU - Gougnaud, F. AU - Gressier, V. AU - Hall-Wilton, R.J. AU - Harrault, F. AU - Höglund, C. AU - Iguaz Gutierrez, F. J. AU - Joannem, T.J. AU - Kebbiri, M. AU - Lahonde-Hamdoun, C. AU - Le Bourlout, P. AU - Legou, Ph. AU - Maillard, O. AU - Marcel, A. AU - Marchand, C. AU - Mariette, Y. AU - Marroncle, J. AU - Nadot, V. AU - Nikolopoulos, K. AU - Oublaid, M. AU - Perreu, G. AU - Piquet, O. AU - Pomorski, M. AU - Pottin, B. AU - Robinson, L. AU - Sauce, Y. AU - Schwindling, J. AU - Segui, L. AU - Senée, F. AU - Shea, T.J. AU - Svensson, P. AU - Touzery, R. AU - Tsiledakis, G. AU - Tuske, O. AU - Uriot, D. ED - Schaa, Volker RW TI - ESS nBLM: Beam Loss Monitors based on Fast Neutron Detection J2 - Proc. of HB2018, Daejeon, Korea, 17-22 June 2018 C1 - Daejeon, Korea T2 - ICFA Advanced Beam Dynamics Workshop T3 - 61 LA - english AB - A new type of Beam Loss Monitor (BLM) system is being developed for use in the European Spallation Source (ESS) linac, primarily aiming to cover the low energy part (proton energies between 3-100 MeV). In this region of the linac, typical BLM detectors based on charged particle detection (i.e. Ionization Cham-bers) are not appropriate because the expected particle fields will be dominated by neutrons and photons. Another issue is the photon background due to the RF cavities, which is mainly due to field emission from the electrons from the cavity walls, resulting in brems-strahlung photons. The idea for the ESS neutron sensi-tive BLM system (ESS nBLM) is to use Micromegas detectors specially designed to be sensitive to fast neutrons and insensitive to low energy photons (X and gammas). In addition, the detectors must be insensitive to thermal neutrons, because those neutrons may not be directly correlated to beam losses. The appropriate configuration of the Micromegas operating conditions will allow excellent timing, intrinsic photon back-ground suppression and individual neutron counting, extending thus the dynamic range to very low particle fluxes. PB - JACoW Publishing CP - Geneva, Switzerland SP - 404 EP - 409 KW - detector KW - neutron KW - linac KW - proton KW - photon DA - 2018/07 PY - 2018 SN - 978-3-95450-202-8 DO - 10.18429/JACoW-HB2018-THA1WE04 UR - http://jacow.org/hb2018/papers/tha1we04.pdf ER -