Issue |
EPJ Web Conf.
Volume 239, 2020
ND 2019: International Conference on Nuclear Data for Science and Technology
|
|
---|---|---|
Article Number | 01024 | |
Number of page(s) | 5 | |
Section | Nuclear Reaction Measurements | |
DOI | https://doi.org/10.1051/epjconf/202023901024 | |
Published online | 30 September 2020 |
https://doi.org/10.1051/epjconf/202023901024
Monte Carlo simulations and n-p differential scattering data measured with Proton Recoil Telescopes
1 Agenzia nazionale per le nuove tecnologie, l’energia e lo sviluppo economico sostenibile (ENEA), Frascati, Italy
2 Istituto Nazionale di Fisica Nucleare, CNAF, Bologna, Italy
3 European Organization for Nuclear Research (CERN), Switzerland
4 Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Spain
5 INFN Laboratori Nazionali del Sud, Catania, Italy
6 Dipartimento di Fisica e Astronomia, Università di Catania, Italy
7 University of Lodz, Poland
8 IPN, CNRS-IN2P3, Univ. Paris-Sud, Université Paris-Saclay, F-91406 Orsay Cedex, France
9 Instituto de Física Corpuscular, CSIC - Universidad de Valencia, Spain
10 Technische Universität Wien, Austria
11 CEA Saclay, Irfu, Université Paris-Saclay, Gif-sur-Yvette, France
12 Istituto Nazionale di Fisica Nucleare, Bari, Italy
13 University of Manchester, United Kingdom
14 Department of Physics, Faculty of Science, University of Zagreb, Croatia
15 University of York, United Kingdom
16 Istituto Nazionale di Fisica Nazionale, Perugia, Italy
17 Dipartimento di Fisica e Geologia, Università di Perugia, Italy
18 University of Santiago de Compostela, Spain
19 Universitat Politècnica de Catalunya, Spain
20 Universidad de Sevilla, Spain
21 Istituto Nazionale di Astrofisica - Osservatorio Astronomico d’Abruzzo, Italy
22 Dipartimento di Fisica, Università degli Studi di Bari, Italy
23 National Technical University of Athens, Greece
24 School of Physics and Astronomy, University of Edinburgh, United Kingdom
25 Paul Scherrer Institut (PSI), Villigen, Switzerland
26 Physikalisch-Technische Bundesanstalt (PTB), Bundesallee 100, 38116 Braunschweig, Germany
27 University of Ioannina, Greece
28 Instituto Superior Técnico, Lisbon, Portugal
29 Joint Institute for Nuclear Research (JINR), Dubna, Russia
30 Goethe University Frankfurt, Germany
31 European Commission, Joint Research Centre, Geel, Retieseweg 111, B-2440 Geel, Belgium
32 Helmholtz-Zentrum Dresden-Rossendorf, Germany
33 Karlsruhe Institute of Technology, Campus North, IKP, 76021 Karlsruhe, Germany
34 Japan Atomic Energy Agency (JAEA), Tokai-mura, Japan
35 Charles University, Prague, Czech Republic
36 Istituto Nazionale di Fisica Nucleare, Sezione di Bologna, Italy
37 Dipartimento di Fisica e Astronomia, Università di Bologna, Italy
38 Istituto Nazionale di Fisica Nucleare, Sezione di Legnaro, Italy
39 Consiglio Nazionale delle Ricerche, Bari, Italy
40 Agenzia nazionale per le nuove tecnologie, l’energia e lo sviluppo economico sostenibile (ENEA), Bologna, Italy
41 Istituto Nazionale di Fisica Nazionale, Trieste, Italy
42 Horia Hulubei National Institute of Physics and Nuclear Engineering (IFIN-HH), Bucharest
43 University of Granada, Spain
44 University of Vienna, Faculty of Physics, Vienna, Austria
45 Bhabha Atomic Research Centre (BARC), India
46 Gran Sasso Science Institute (GSSI), L’Aquila, Italy
47 Australian National University, Canberra, Australia
* e-mail: nicholas.terranova@enea.it
Published online: 30 September 2020
The neutron-induced fission cross section of 235U, a standard at thermal energy and between 0.15 MeV and 200 MeV, plays a crucial role in nuclear technology applications. The long-standing need of improving cross section data above 20 MeV and the lack of experimental data above 200 MeV motivated a new experimental campaign at the n_TOF facility at CERN. The measurement has been performed in 2018 at the experimental area 1 (EAR1), located at 185 m from the neutron-producing target (the experiment is presented by A. Manna et al. in a contribution to this conference). The 235U(n,f) cross section from 20 MeV up to about 1 GeV has been measured relative to the 1H(n,n)1H reaction, which is considered the primary reference in this energy region. The neutron flux impinging on the 235U sample (a key quantity for determining the fission events) has been obtained by detecting recoil protons originating from n-p scattering in a C2H4 sample. Two Proton Recoil Telescopes (PRT), consisting of several layers of solid-state detectors and fast plastic scintillators, have been located at proton scattering angles of 25.07° and 20.32°, out of the neutron beam. The PRTs exploit the ΔE-E technique for particle identification, a basic requirement for the rejection of charged particles from neutron-induced reactions in carbon. Extensive Monte Carlo simulations were performed to characterize proton transport through the different slabs of silicon and scintillation detectors, to optimize the experimental set-up and to deduce the efficiency of the whole PRT detector. In this work we compare measured data collected with the PRTs with a full Monte Carlo simulation based on the Geant-4 toolkit.
© The Authors, published by EDP Sciences, 2020
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