Experimental setup and procedure for the measurement of the 7Be(n,p)7Li reaction at n_TOF
M. Barbagallo, J. Andrzejewski, M. Mastromarco, J. Perkowski, L. A. Damone, A. Gawlik, L. Cosentino, P. Finocchiaro, E. A. Maugeri, A. Mazzone, R. Dressler, S. … 展开作者
M. Barbagallo, J. Andrzejewski, M. Mastromarco, J. Perkowski, L. A. Damone, A. Gawlik, L. Cosentino, P. Finocchiaro, E. A. Maugeri, A. Mazzone, R. Dressler, S. Heinitz, N. Kivel, D. Schumann, N. Colonna, O. Aberle, S. Amaducci, L. Audouin, M. Bacak, J. Balibrea, F. Bečvář, G. Bellia, E. Berthoumieux, J. Billowes, D. Bosnar, A. Brown, M. Caamaño, F. Calviño, M. Calviani, D. Cano-Ott, R. Cardella, A. Casanovas, F. Cerutti, Y. H. Chen, E. Chiaveri, G. Cortés, M. A. Cortés-Giraldo, S. Cristallo, M. Diakaki, M. Dietz, C. Domingo-Pardo, E. Dupont, I. Durán, B. Fernández-Domínguez, A. Ferrari, P. Ferreira, V. Furman, K. Göbel, A. R. García, S. Gilardoni, T. Glodariu, I. F. Gonçalves, E. González-Romero, E. Griesmayer, C. Guerrero, F. Gunsing, H. Harada, J. Heyse, D. G. Jenkins, E. Jericha, K. Johnston, F. Käppeler, Y. Kadi, A. Kalamara, P. Kavrigin, A. Kimura, M. Kokkoris, M. Krtička, D. Kurtulgil, C. Lederer, H. Leeb, J. Lerendegui-Marco, S. Lo Meo, S. J. Lonsdale, D. Macina, A. Manna, J. Marganiec, T. Martínez, J. G. Martins-Correia, A. Masi, C. Massimi, P. Mastinu, E. Mendoza, A. Mengoni, P. M. Milazzo, F. Mingrone, A. Musumarra, A. Negret, R. Nolte, A. Oprea, A. D. Pappalardo, N. Patronis, A. Pavlik, M. Piscopo, I. Porras, J. Praena, J. M. Quesada, D. Radeck, T. Rauscher, R. Reifarth, M. S. Robles, C. Rubbia, J. A. Ryan, M. Sabaté-Gilarte, A. Saxena, J. Schell, P. Schillebeeckx, P. Sedyshev, A. G. Smith, N. V. Sosnin, A. Stamatopoulos, G. Tagliente, J. L. Tain, A. Tarifeño-Saldivia, L. Tassan-Got, S. Valenta, G. Vannini, V. Variale, P. Vaz, A. Ventura, V. Vlachoudis, R. Vlastou, A. Wallner, S. Warren, C. Weiss, P. J. Woods, T. Wright, P. Žugec
Following the completion of the second neutron beam line and the related experimental area (EAR2) at the n_TOF spallation neutron source at CERN, several experiments were planned and performed. The high instantaneous neutron flux available in EAR2 allows to investigate neutron indiced reactions with charged particles in the exit channel even employing targets made out of small amounts of short-lived radioactive isotopes. After the successful measurement of the 7Be(n,α)α cross section, the 7Be(n,p)7Li reaction was studied in order to provide still missing cross section data of relevance for Big Bang Nucleosynthesis (BBN), in an attempt to find a solution to the cosmological Lithium abundance problem. This paper describes the experimental setup employed in such a measurement and its characterization.
Recoil Proton Telescopes and Parallel Plate Avalanche Counters for the $^{235}$U(n,f) cross section measurement relative to H(n,n)H between 10 and 450 MeV neutron energy
Surrogate neutron-capture studies with fission detection in inverse kinematics at the ESR storage ring
Université de Bordeaux（波尔多大学）；CNRS（法国国家科学研究中心）；LP2I Bordeaux（波尔多光电与离子研究所）；Max-Planck-Institut fur Kernphysik（马克斯·普朗克核物理研究所）；GSI Helmholtzzentrum fur Schwerionenforschung（德国重离子研究中心）；Universität zu Köln（科隆大学）；Université Paris-Saclay（巴黎萨克雷大学）；IJCLab（伊夫林-约瑟夫·朗之万实验室）；GANIL（法国国家重离子加速器中心）；CRNS/IN2P3-CEA/DRF（法国国家科研中心/法国国家原子能委员会）；Université de Caen-Normandie（诺曼底卡昂大学）；Goethe Universitat Frankfurt（法兰克福歌德大学）；Commissariat à l’énergie atomique et aux énergies alternatives（法国原子能和替代能源委员会）
