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Design of the third-generation lead-based neutron spallation target for the neutron time-of-flight facility at CERN

R. Esposito, M. Calviani, O. Aberle, M. Barbagallo, D. Cano-Ott, T. Coiffet, N. Colonna, C. Domingo-Pardo, F. Dragoni, R. Franqueira Ximenes, L. Giordanino, D. Grenier, F. Gunsing, K. Kershaw, R. Logé, V. Maire, P. Moyret, A. Perez Fontenla, A. Perillo-Marcone, F. Pozzi, S. Sgobba, M. Timmins, and V. Vlachoudis (for the n_TOF Collaboration)
Phys. Rev. Accel. Beams 24, 093001 – Published 7 September 2021

Abstract

The neutron time-of-flight (n_TOF) facility at the European Laboratory for Particle Physics (CERN) is a pulsed white-spectrum neutron spallation source producing neutrons for two experimental areas: the Experimental Area 1 (EAR1), located 185 m horizontally from the target, and the Experimental Area 2 (EAR2), located 20 m above the target. The target, based on pure lead, is impacted by a high-intensity 20GeV/c pulsed proton beam. The facility was conceived to study neutron-nucleus interactions for neutron kinetic energies between a few meV to several GeV, with applications of interest for nuclear astrophysics, nuclear technology, and medical research. After the second-generation target reached the end of its lifetime, the facility underwent a major upgrade during CERN’s Long Shutdown 2 (LS2, 2019–2021), which included the installation of the new third-generation neutron target. The first- and second-generation targets were based on water-cooled massive lead blocks and were designed focusing on EAR1, since EAR2 was built later. The new target is cooled by nitrogen gas to avoid erosion-corrosion and contamination of cooling water with radioactive lead spallation products. Moreover, the new design is optimized also for the vertical flight path and EAR2. This paper presents an overview of the target design focused on both physics and thermomechanical performance, and includes a description of the nitrogen cooling circuit and radiation protection studies.

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  • Received 22 June 2021
  • Accepted 13 August 2021
  • Corrected 26 May 2022

DOI:https://doi.org/10.1103/PhysRevAccelBeams.24.093001

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Accelerators & Beams

Corrections

26 May 2022

Correction: The previously published Fig. 8 contained an error in the abscissa units and has been replaced.

Authors & Affiliations

R. Esposito1,2,*, M. Calviani1,†, O. Aberle1, M. Barbagallo1, D. Cano-Ott3, T. Coiffet1, N. Colonna4, C. Domingo-Pardo5, F. Dragoni1, R. Franqueira Ximenes1, L. Giordanino1, D. Grenier1, F. Gunsing6, K. Kershaw1, R. Logé2, V. Maire1, P. Moyret1, A. Perez Fontenla1, A. Perillo-Marcone1, F. Pozzi1, S. Sgobba1, M. Timmins1, and V. Vlachoudis1 (for the n_TOF Collaboration)

  • 1European Laboratory for Particle Physics (CERN), 1211 Geneva 23, Switzerland
  • 2Thermomechanical Metallurgy Laboratory, PX Group Chair, Ecole Polytechnique Fédérale de Lausanne (EPFL), 2002 Neuchâtel, Switzerland
  • 3Centro de Investigaciones Energéticas Medioambientales y Tecnológicas, Madrid, Spain
  • 4Istituto Nazionale di Fisica Nucleare, Bari, Italy
  • 5Instituto de Física Corpuscular, CSIC-Universitat de Valencia, Spain
  • 6CEA Saclay, Irfu, Gif-sur-Yvette, France

  • *raffaele.esposito@cern.ch
  • marco.calviani@cern.ch

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Issue

Vol. 24, Iss. 9 — September 2021

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