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Achieving ultra-low and -uniform residual magnetic fields in a very large magnetically shielded room for fundamental physics experiments.
Ayres, N J; Ban, G; Bison, G; Bodek, K; Bondar, V; Bouillaud, T; Bowles, D; Chanel, E; Chen, W; Chiu, P-J; Crawford, C B; Naviliat-Cuncic, O; Doorenbos, C B; Emmenegger, S; Fertl, M; Fratangelo, A; Griffith, W C; Grujic, Z D; Harris, P G; Kirch, K; Kletzl, V; Krempel, J; Lauss, B; Lefort, T; Lejuez, A; Li, R; Mullan, P; Pacura, S; Pais, D; Piegsa, F M; Rienäcker, I; Ries, D; Pignol, G; Rebreyend, D; Roccia, S; Rozpedzik, D; Saenz-Arevalo, W; Schmidt-Wellenburg, P; Schnabel, A; Segarra, E P; Severijns, N; Svirina, K; Tavakoli Dinani, R; Thorne, J; Vankeirsbilck, J; Voigt, J; Yazdandoost, N; Zejma, J; Ziehl, N; Zsigmond, G.
Affiliation
  • Ayres NJ; Institute for Particle Physics and Astrophysics, ETH Zürich, 8093 Zurich, Switzerland.
  • Ban G; Normandie Université, ENSICAEN, UNICAEN, CNRS/IN2P3, LPC Caen, 14000 Caen, France.
  • Bison G; Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Bodek K; Marian Smoluchowski Institute of Physics, Jagiellonian University, 30-348 Kraków, Poland.
  • Bondar V; Institute for Particle Physics and Astrophysics, ETH Zürich, 8093 Zurich, Switzerland.
  • Bouillaud T; Université Grenoble Alpes, CNRS, Grenoble INP, LPSC-IN2P3, 38026 Grenoble, France.
  • Bowles D; Department of Physics and Astronomy, University of Kentucky, Lexington, KY 40506 USA.
  • Chanel E; Laboratory for High Energy Physics and Albert Einstein Center for Fundamental Physics, University of Bern, 3012 Bern, Switzerland.
  • Chen W; Institute for Particle Physics and Astrophysics, ETH Zürich, 8093 Zurich, Switzerland.
  • Chiu PJ; Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Crawford CB; University of Zürich, 8057 Zurich, Switzerland.
  • Naviliat-Cuncic O; Department of Physics and Astronomy, University of Kentucky, Lexington, KY 40506 USA.
  • Doorenbos CB; Normandie Université, ENSICAEN, UNICAEN, CNRS/IN2P3, LPC Caen, 14000 Caen, France.
  • Emmenegger S; Institute for Particle Physics and Astrophysics, ETH Zürich, 8093 Zurich, Switzerland.
  • Fertl M; Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Fratangelo A; Institute for Particle Physics and Astrophysics, ETH Zürich, 8093 Zurich, Switzerland.
  • Griffith WC; Institute of Physics, Johannes Gutenberg University, 55128 Mainz, Germany.
  • Grujic ZD; Laboratory for High Energy Physics and Albert Einstein Center for Fundamental Physics, University of Bern, 3012 Bern, Switzerland.
  • Harris PG; Department of Physics and Astronomy, University of Sussex, Falmer, Brighton, BN1 9QH UK.
  • Kirch K; Institute of Physics, Photonics Center, University of Belgrade, Belgrade, 11080 Serbia.
  • Kletzl V; Department of Physics and Astronomy, University of Sussex, Falmer, Brighton, BN1 9QH UK.
  • Krempel J; Institute for Particle Physics and Astrophysics, ETH Zürich, 8093 Zurich, Switzerland.
  • Lauss B; Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Lefort T; Institute for Particle Physics and Astrophysics, ETH Zürich, 8093 Zurich, Switzerland.
  • Lejuez A; Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Li R; Institute for Particle Physics and Astrophysics, ETH Zürich, 8093 Zurich, Switzerland.
  • Mullan P; Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Pacura S; Normandie Université, ENSICAEN, UNICAEN, CNRS/IN2P3, LPC Caen, 14000 Caen, France.
  • Pais D; Normandie Université, ENSICAEN, UNICAEN, CNRS/IN2P3, LPC Caen, 14000 Caen, France.
  • Piegsa FM; Instituut voor Kern-en Stralingsfysica, University of Leuven, 3001 Leuven, Belgium.
  • Rienäcker I; Institute for Particle Physics and Astrophysics, ETH Zürich, 8093 Zurich, Switzerland.
  • Ries D; Marian Smoluchowski Institute of Physics, Jagiellonian University, 30-348 Kraków, Poland.
  • Pignol G; Institute for Particle Physics and Astrophysics, ETH Zürich, 8093 Zurich, Switzerland.
  • Rebreyend D; Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Roccia S; Laboratory for High Energy Physics and Albert Einstein Center for Fundamental Physics, University of Bern, 3012 Bern, Switzerland.
  • Rozpedzik D; Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Saenz-Arevalo W; Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Schmidt-Wellenburg P; Université Grenoble Alpes, CNRS, Grenoble INP, LPSC-IN2P3, 38026 Grenoble, France.
  • Schnabel A; Université Grenoble Alpes, CNRS, Grenoble INP, LPSC-IN2P3, 38026 Grenoble, France.
  • Segarra EP; Université Grenoble Alpes, CNRS, Grenoble INP, LPSC-IN2P3, 38026 Grenoble, France.
  • Severijns N; Marian Smoluchowski Institute of Physics, Jagiellonian University, 30-348 Kraków, Poland.
  • Svirina K; Normandie Université, ENSICAEN, UNICAEN, CNRS/IN2P3, LPC Caen, 14000 Caen, France.
  • Tavakoli Dinani R; Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Thorne J; Physikalisch-Technische Bundesanstalt, Abbestr. 2-12, 10587 Berlin, Germany.
  • Vankeirsbilck J; Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.
  • Voigt J; Instituut voor Kern-en Stralingsfysica, University of Leuven, 3001 Leuven, Belgium.
  • Yazdandoost N; Université Grenoble Alpes, CNRS, Grenoble INP, LPSC-IN2P3, 38026 Grenoble, France.
  • Zejma J; Instituut voor Kern-en Stralingsfysica, University of Leuven, 3001 Leuven, Belgium.
  • Ziehl N; Laboratory for High Energy Physics and Albert Einstein Center for Fundamental Physics, University of Bern, 3012 Bern, Switzerland.
  • Zsigmond G; Instituut voor Kern-en Stralingsfysica, University of Leuven, 3001 Leuven, Belgium.
Eur Phys J C Part Fields ; 84(1): 18, 2024.
Article in En | MEDLINE | ID: mdl-38205101
ABSTRACT
High-precision searches for an electric dipole moment of the neutron (nEDM) require stable and uniform magnetic field environments. We present the recent achievements of degaussing and equilibrating the magnetically shielded room (MSR) for the n2EDM experiment at the Paul Scherrer Institute. We present the final degaussing configuration that will be used for n2EDM after numerous studies. The optimized procedure results in a residual magnetic field that has been reduced by a factor of two. The ultra-low field is achieved with the full magnetic-field-coil system, and a large vacuum vessel installed, both in the MSR. In the inner volume of ∼1.4m3, the field is now more uniform and below 300 pT. In addition, the procedure is faster and dissipates less heat into the magnetic environment, which in turn, reduces its thermal relaxation time from 12h down to 1.5h.