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3 results on '"D. Körper"'

1. NeuLAND: The high-resolution neutron time-of-flight spectrometer for R3B at FAIR

Author

M.I. Cherciu, N.G. Kozlenko, Andreas Martin Heinz, P. Russotto, Christoph Langer, Z. Elekes, Nasser Kalantar-Nayestanaki, G. Ickert, Thomas Aumann, Thomas Nilsson, L. Zanetti, M. Volknandt, E. M. Orischin, Heiko Scheit, K. Koch, E.V. Pagano, V. Kuznetsov, S. Chakraborty, U. Datta, V. L. Golovtsov, N. Kurz, E. Hoemann, Tanja Heftrich, S. S. Volkov, J. Dreyer, M. Kempe, D. M. Rossi, T. Hensel, A. Horvat, C. Caesar, V. Wagner, G. Politi, I. Lihtar, F. Schindler, B. Löher, Ahibur Rahaman, Catherine Rigollet, J. Kahlbow, H. Törnqvist, A. Kelic-Heil, Herbert A. Simon, Daniel Stach, E. De Filippo, D. Galaviz, N. S. Martorana, Daniel Bemmerer, D. Gonzalez Diaz, D. Körper, Jorge Machado, E. Stan, B. Gnoffo, L. V. Chulkov, P. Teubig, N. Gruzinsky, J. Mayer, G. Alkhazov, J. Hehner, Rene Reifarth, S. Wranne, S. Pirrone, Håkan T Johansson, K. Miki, Lukas Bott, E. Geraci, K. Boretzky, I. Gašparić, H. Heggen, D. Kresan, M. Trimarchi, Kathrin Göbel, D. Jelavić Malenica, J. Stomvall Gill, S.V. Bondarev, M. Holl, Andreas Zilges, D. Yakorev, Joachim Enders, L. Atar, P.-M. Potlog, L. Uvarov, Björn Jonson, Andreas Wagner, Matthias Heil, M. Ciobanu, Á. Horváth, A.G. Krivshich, M. Röder, C.A. Douma, Y. Leifels, Deniz Savran, Kai Zuber, Research unit Nuclear & Hadron Physics, and Nuclear Energy

Subjects
Physics, Nuclear and High Energy Physics, Spectrometer, business.industry, High-energy neutron detection, Reactions with relativistic radioactive beams, Plastic scintillator array, Multi-neutron detection, Detector, Scintillator, Time of flight, Optics, Neutron detection, Facility for Antiproton and Ion Research, Neutron, ddc:530, Nuclear Experiment, business, Instrumentation, Image resolution
Abstract

Nuclear instruments & methods in physics research / A 1014, 165701 (2021). doi:10.1016/j.nima.2021.165701, Published by North-Holland Publ. Co., Amsterdam

Published
2021
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2. Performance of timing resistive plate chambers with relativistic neutrons from 300 to 1500 MeV

Author

M. Pohl, Rene Reifarth, B. Löher, L. Lopes, Daniel Stach, G. Rastrepina, M. Holl, M. Heine, J. Marganiec, D. M. Rossi, Daniel Bemmerer, J. Fruehauf, A. Kelic-Heil, P. Schrock, J. Silva, Deniz Savran, D. Galaviz, Stefanos Paschalis, Andreas Martin Heinz, Mario Weigand, M. Traxler, P. Teubig, Z. Elekes, P. Velho, Marek Palka, R. Thies, Jorge Machado, Marina Petri, L. Cartegni, D. Körper, Tanja Heftrich, C. Caesar, V. Panin, J. Isaak, A. Henriques, Simon Lindberg, C. Lederer, A. Blanco, A. Pereira, P. Fonte, Thomas Nilsson, S. Altstadt, Kathrin Göbel, F. Wamers, T. P. Reinhardt, Thomas Aumann, J. Gerbig, G. Ickert, Heiko Scheit, Mikael Mårtensson, A. Ignatov, Igor Gašparić, Håkan T Johansson, Fredrik Strannerdahl, Ralf Plag, E. Fiori, K. Boretzky, R. Ferreira Marques, L. Atar, J. Adamczewski-Musch, P. Cabanelas, H. Simon, Matthias Heil, M. Röder, Andreas Wagner, and Alexandre Charpy

Subjects
Resistive touchscreen, Materials science, business.industry, Aucun, Float glass, Glass electrode, Neutron temperature, law.invention, Time of flight, Nuclear magnetic resonance, Optics, law, Electrode, Neutron, business, Instrumentation, Mathematical Physics, Beam (structure)
Abstract

A prototype composed of four resistive plate chamber layers has been exposed to quasi-monoenergetic neutrons produced from a deuteron beam of varying energy (300 to 1500 AMeV) in experiment S406 at GSI, Darmstad, Germany. Each layer, with an active area of about 2000 × 500 mm2, is made of modules containing the active gaps, all in multigap construction. Each gap is defined by 0.3 mm nylon mono-filaments positioned between 2.85 mm thick float glass electrodes. The modules are operated in avalanche mode with a non-flammable gas mixture composed of 90% C2H2F4 and 10% SF6. The signals are readout by a pick-up electrode formed by 15 copper strips (per layer), spaced at a pitch of 30 mm, connected at both sides to timing front end electronics. Measurements of the time of flight jitter of neutrons, in the mentioned energy range, point to a contribution of the resistive plate chamber in the order of 150 ps, independent of the neutron energy.

Published
2015
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3. Performance of timing Resistive Plate Chambers with protons from 200 to 800 MeV

Author

D. M. Rossi, Mario Weigand, Simon Lindberg, Rene Reifarth, T. P. Reinhardt, J. Isaak, M. Heine, Z. Elekes, A. Henriques, R. Thies, Daniel Bemmerer, Jorge Machado, Thomas Nilsson, J. Marganiec, Marina Petri, G. Ickert, B. Löher, L. Lopes, L. Cartegni, D. Körper, A. Blanco, P. Fonte, Stefanos Paschalis, Heiko Scheit, F. Wamers, Daniel Stach, M. Traxler, E. Fiori, A. Ignatov, Thomas Aumann, Håkan T Johansson, J. Gerbig, G. Rastrepina, J. Silva, Fredrik Strannerdahl, J. Fruehauf, Mikael Mårtensson, Ralf Plag, Andreas Martin Heinz, A. Kelic-Heil, Tanja Heftrich, A. Pereira, D. Galaviz, K. Boretzky, P. Teubig, Kathrin Göbel, Igor Gašparić, P. Schrock, V. Panin, S. Altstadt, H. Simon, M. Pohl, L. Atar, P. Velho, P. Cabanelas, Matthias Heil, J. Adamczewski-Musch, M. Röder, Andreas Wagner, Alexandre Charpy, M. Holl, Deniz Savran, R. Ferreira Marques, Marek Palka, C. Lederer, and C. Caesar

Subjects
Range (particle radiation), Resistive touchscreen, Materials science, business.industry, Electrical engineering, Float glass, STRIPS, 7. Clean energy, Glass electrode, Particle detector, law.invention, Optics, law, Electrode, business, Instrumentation, Mathematical Physics, Beam (structure)
Abstract

A prototype composed of four resistive plate chamber layers has been exposed to quasi-monoenergetic protons produced from a deuteron beam of varying energy (200 to 800 AMeV) in experiment S406 at GSI, Darmstadt, Germany. The aim of the experiment is to characterize the response of the prototype to protons in this energy range, which deposit from 1.75 to 6 times more energy than minimum ionizing particles. Each layer, with an active area of about 2000 × 500 mm2, is made of modules containing the active gaps, all in multigap construction. Each gap is defined by 0.3 mm nylon mono-filaments positioned between 2.85 mm thick float glass electrodes. The modules are operated in avalanche mode with a non-flammable gas mixture composed of 90% C2H2F4 and 10% SF6. The signals are readout by a pick-up electrode formed by 15 copper strips (per layer), spaced at a pitch of 30 mm, connected at both sides to timing front end electronics. Results show an uniform efficiency close to 100% along with a timing resolution of around 60 ps on the entire 2000 × 500 mm2 area.

Published
2015
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