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A large 'Active Magnetic Shield' for a high-precision experiment: nEDM collaboration.
Abel, C; Ayres, N J; Ban, G; Bison, G; Bodek, K; Bondar, V; Bouillaud, T; Chanel, E; Chen, J; Chen, W; Chiu, P-J; Crawford, C B; Daum, M; Doorenbos, C B; Emmenegger, S; Ferraris-Bouchez, L; Fertl, M; Fratangelo, A; Griffith, W C; Grujic, Z D; Harris, P; Kirch, K; Kletzl, V; Koss, P A; Krempel, J; Lauss, B; Lefort, T; Mullan, P; Naviliat-Cuncic, O; Pais, D; Piegsa, F M; Pignol, G; Rawlik, M; Rienäcker, I; Ries, D; Roccia, S; Rozpedzik, D; Saenz-Arevalo, W; Schmidt-Wellenburg, P; Schnabel, A; Segarra, E P; Severijns, N; Shelton, T; Svirina, K; Tavakoli Dinani, R; Thorne, J; Virot, R; Yazdandoost, N; Zejma, J; Ziehl, N.
Afiliación
  • Abel C; Department of Physics and Astronomy, University of Sussex, Falmer, Brighton, BN1 9QH UK.
  • Ayres NJ; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Ban G; Normandie Univ, ENSICAEN, UNICAEN, CNRS/IN2P3, LPC Caen, 14000 Caen, France.
  • Bison G; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Bodek K; Marian Smoluchowski Institute of Physics, Jagiellonian University, 30-348 Cracow, Poland.
  • Bondar V; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Bouillaud T; LPSC, Université Grenoble Alpes, CNRS/IN2P3, Grenoble, France.
  • Chanel E; University of Bern, Albert Einstein Center for Fundamental Physics, 3012 Bern, Switzerland.
  • Chen J; Present Address: Institut Laue Langevin, 71 avenue des Martyrs CS 20156, 38042 Grenoble Cedex 9, France.
  • Chen W; Normandie Univ, ENSICAEN, UNICAEN, CNRS/IN2P3, LPC Caen, 14000 Caen, France.
  • Chiu PJ; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Crawford CB; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Daum M; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Doorenbos CB; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Emmenegger S; Present Address: University of Zurich, 8057 Zurich, Switzerland.
  • Ferraris-Bouchez L; University of Kentucky, Lexington, USA.
  • Fertl M; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Fratangelo A; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Griffith WC; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Grujic ZD; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Harris P; Present Address: Hochschule Luzern, 6002 Luzern, Switzerland.
  • Kirch K; LPSC, Université Grenoble Alpes, CNRS/IN2P3, Grenoble, France.
  • Kletzl V; Institute of Physics, Johannes Gutenberg University, 55128 Mainz, Germany.
  • Koss PA; University of Bern, Albert Einstein Center for Fundamental Physics, 3012 Bern, Switzerland.
  • Krempel J; Department of Physics and Astronomy, University of Sussex, Falmer, Brighton, BN1 9QH UK.
  • Lauss B; Institute of Physics Belgrade, University of Belgrade, 11080 Belgrade, Serbia.
  • Lefort T; Department of Physics and Astronomy, University of Sussex, Falmer, Brighton, BN1 9QH UK.
  • Mullan P; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Naviliat-Cuncic O; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Pais D; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Piegsa FM; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Pignol G; Institute for Nuclear and Radiation Physics, KU Leuven, 3001 Leuven, Belgium.
  • Rawlik M; Present Address: Fraunhofer Institute for Physical Measurement Techniques, 79110 Freiburg, Germany.
  • Rienäcker I; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Ries D; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Roccia S; Normandie Univ, ENSICAEN, UNICAEN, CNRS/IN2P3, LPC Caen, 14000 Caen, France.
  • Rozpedzik D; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Saenz-Arevalo W; Normandie Univ, ENSICAEN, UNICAEN, CNRS/IN2P3, LPC Caen, 14000 Caen, France.
  • Schmidt-Wellenburg P; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Schnabel A; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Segarra EP; University of Bern, Albert Einstein Center for Fundamental Physics, 3012 Bern, Switzerland.
  • Severijns N; LPSC, Université Grenoble Alpes, CNRS/IN2P3, Grenoble, France.
  • Shelton T; ETH Zürich, Institute for Particle Physics and Astrophysics, 8093 Zurich, Switzerland.
  • Svirina K; Present Address: Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Tavakoli Dinani R; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Thorne J; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
  • Virot R; LPSC, Université Grenoble Alpes, CNRS/IN2P3, Grenoble, France.
  • Yazdandoost N; Marian Smoluchowski Institute of Physics, Jagiellonian University, 30-348 Cracow, Poland.
  • Zejma J; Normandie Univ, ENSICAEN, UNICAEN, CNRS/IN2P3, LPC Caen, 14000 Caen, France.
  • Ziehl N; Paul Scherrer Institut (PSI), 5232 Villigen, Switzerland.
Eur Phys J C Part Fields ; 83(11): 1061, 2023.
Article en En | MEDLINE | ID: mdl-38021215
ABSTRACT
We present a novel Active Magnetic Shield (AMS), designed and implemented for the n2EDM experiment at the Paul Scherrer Institute. The experiment will perform a high-sensitivity search for the electric dipole moment of the neutron. Magnetic-field stability and control is of key importance for n2EDM. A large, cubic, 5 m side length, magnetically shielded room (MSR) provides a passive, quasi-static shielding-factor of about 105 for its inner sensitive volume. The AMS consists of a system of eight complex, feedback-controlled compensation coils constructed on an irregular grid spanned on a volume of less than 1000 m3 around the MSR. The AMS is designed to provide a stable and uniform magnetic-field environment around the MSR, while being reasonably compact. The system can compensate static and variable magnetic fields up to ±50µT (homogeneous components) and ±5µT/m (first-order gradients), suppressing them to a few µT in the sub-Hertz frequency range. The presented design concept and implementation of the AMS fulfills the requirements of the n2EDM experiment and can be useful for other applications, where magnetically silent environments are important and spatial constraints inhibit simpler geometrical solutions.

Texto completo: 1 Banco de datos: MEDLINE Idioma: En Revista: Eur Phys J C Part Fields Año: 2023 Tipo del documento: Article

Texto completo: 1 Banco de datos: MEDLINE Idioma: En Revista: Eur Phys J C Part Fields Año: 2023 Tipo del documento: Article