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  • Access by Xinjiang University

Search for the production of Higgs-portal scalar bosons in the NuMI beam using the MicroBooNE detector

P. Abratenko38, D. Andrade Aldana14, L. Arellano21, J. Asaadi37, A. Ashkenazi36, S. Balasubramanian12, B. Baller12, A. Barnard28, G. Barr28 et al. (The MicroBooNE Collaboration*)

G. Barr28, D. Barrow28, J. Barrow25, V. Basque12, J. Bateman21, O. Benevides Rodrigues14, S. Berkman24, A. Bhanderi21, A. Bhat7, M. Bhattacharya12, M. Bishai3, A. Blake18, B. Bogart23, T. Bolton17, M. B. Brunetti40, L. Camilleri10, D. Caratelli4, F. Cavanna12, G. Cerati12, A. Chappell40, Y. Chen32, J. M. Conrad22, M. Convery32, L. Cooper-Troendle29, J. I. Crespo-Anadón6, R. Cross40, M. Del Tutto12, S. R. Dennis5, P. Detje5, R. Diurba2, Z. Djurcic1, K. Duffy28, S. Dytman29, B. Eberly34, P. Englezos31, A. Ereditato7,12, J. J. Evans21, C. Fang4, W. Foreman14,19, B. T. Fleming7, D. Franco7, A. P. Furmanski25, F. Gao4, D. Garcia-Gamez13, S. Gardiner12, G. Ge10, S. Gollapinni19, E. Gramellini21, P. Green28, H. Greenlee12, L. Gu18, W. Gu3, R. Guenette21, P. Guzowski21, L. Hagaman7, M. D. Handley5, O. Hen22, C. Hilgenberg25, G. A. Horton-Smith17, B. Irwin25, M. S. Ismail29, C. James12, X. Ji26, J. H. Jo3, R. A. Johnson8, Y.-J. Jwa10, D. Kalra10, G. Karagiorgi10, W. Ketchum12, M. Kirby3, T. Kobilarcik12, N. Lane21, J.-Y. Li11, Y. Li3, K. Lin31, B. R. Littlejohn14, L. Liu12, W. C. Louis19, X. Luo4, T. Mahmud18, C. Mariani39, D. Marsden21, J. Marshall40, N. Martinez17, D. A. Martinez Caicedo33, S. Martynenko3, A. Mastbaum31, I. Mawby18, N. McConkey30, L. Mellet24, J. Mendez20, J. Micallef22,38, A. Mogan9, T. Mohayai16, M. Mooney9, A. F. Moor5, C. D. Moore12, L. Mora Lepin21, M. M. Moudgalya21, S. Mulleriababu2, D. Naples29, A. Navrer-Agasson15,21, N. Nayak3, M. Nebot-Guinot11, C. Nguyen31, J. Nowak18, N. Oza10, O. Palamara12, N. Pallat25, V. Paolone29, A. Papadopoulou1, V. Papavassiliou27, H. B. Parkinson11, S. F. Pate27, N. Patel18, Z. Pavlovic12, E. Piasetzky36, K. Pletcher24, I. Pophale18, X. Qian3, J. L. Raaf12, V. Radeka3, A. Rafique1, M. Reggiani-Guzzo11, L. Rochester32, J. Rodriguez Rondon33, M. Rosenberg38, M. Ross-Lonergan19, I. Safa10, D. W. Schmitz7, A. Schukraft12, W. Seligman10, M. H. Shaevitz10, R. Sharankova12, J. Shi5, E. L. Snider12, M. Soderberg35, S. Söldner-Rembold15,21, J. Spitz23, M. Stancari12, J. St. John12, T. Strauss12, A. M. Szelc11, N. Taniuchi5, K. Terao32, C. Thorpe21, D. Torbunov3, D. Totani4, M. Toups12, A. Trettin21, Y.-T. Tsai32, J. Tyler17, M. A. Uchida5, T. Usher32, B. Viren3, J. Wang26, M. Weber2, H. Wei20, A. J. White7, S. Wolbers12, T. Wongjirad38, M. Wospakrik12, K. Wresilo5, W. Wu29, E. Yandel4,19, T. Yang12, L. E. Yates12, H. W. Yu3, G. P. Zeller12, J. Zennamo12, and C. Zhang3 (The MicroBooNE Collaboration*)

  • 1Argonne National Laboratory (ANL), Lemont, Illinois 60439, USA
  • 2Universität Bern, Bern CH-3012, Switzerland
  • 3Brookhaven National Laboratory (BNL), Upton, New York 11973, USA
  • 4University of California, Santa Barbara, California 93106, USA
  • 5University of Cambridge, Cambridge CB3 0HE, United Kingdom
  • 6Centro de Investigaciones Energéticas, Medioambientales y Tecnológicas (CIEMAT), Madrid E-28040, Spain
  • 7University of Chicago, Chicago, Illinois 60637, USA
  • 8University of Cincinnati, Cincinnati, Ohio 45221, USA
  • 9Colorado State University, Fort Collins, Colorado 80523, USA
  • 10Columbia University, New York, New York 10027, USA
  • 11University of Edinburgh, Edinburgh EH9 3FD, United Kingdom
  • 12Fermi National Accelerator Laboratory (FNAL), Batavia, Illinois 60510, USA
  • 13Universidad de Granada, Granada E-18071, Spain
  • 14Illinois Institute of Technology (IIT), Chicago, Illinois 60616, USA
  • 15Imperial College London, London SW7 2AZ, United Kingdom
  • 16Indiana University, Bloomington, Indiana 47405, USA
  • 17Kansas State University (KSU), Manhattan, Kansas 66506, USA
  • 18Lancaster University, Lancaster LA1 4YW, United Kingdom
  • 19Los Alamos National Laboratory (LANL), Los Alamos, New Mexico 87545, USA
  • 20Louisiana State University, Baton Rouge, Louisiana 70803, USA
  • 21The University of Manchester, Manchester M13 9PL, United Kingdom
  • 22Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA
  • 23University of Michigan, Ann Arbor, Michigan 48109, USA
  • 24Michigan State University, East Lansing, Michigan 48824, USA
  • 25University of Minnesota, Minneapolis, Minnesota 55455, USA
  • 26Nankai University, Nankai District, Tianjin 300071, China
  • 27New Mexico State University (NMSU), Las Cruces, New Mexico 88003, USA
  • 28University of Oxford, Oxford OX1 3RH, United Kingdom
  • 29University of Pittsburgh, Pittsburgh, Pennsylvania 15260, USA
  • 30Queen Mary University of London, London E1 4NS, United Kingdom
  • 31Rutgers University, Piscataway, New Jersey 08854, USA
  • 32SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
  • 33South Dakota School of Mines and Technology (SDSMT), Rapid City, South Dakota 57701, USA
  • 34University of Southern Maine, Portland, Maine 04104, USA
  • 35Syracuse University, Syracuse, New York 13244, USA
  • 36Tel Aviv University, Tel Aviv, Israel, 69978
  • 37University of Texas, Arlington, Texas 76019, USA
  • 38Tufts University, Medford, Massachusetts 02155, USA
  • 39Center for Neutrino Physics, Virginia Tech, Blacksburg, Virginia 24061, USA
  • 40University of Warwick, Coventry CV4 7AL, United Kingdom

  • *Contact author: microboone_info@fnal.gov

Phys. Rev. D 113, 075007 – Published 6 April, 2026

DOI: https://doi.org/10.1103/6myb-c3g1

Abstract

We present the strongest experimental limits to date on the mixing angle, θ, with which a new scalar particle, S, mixes with the Higgs field in the mass range 110MeV<mS<155MeV. This result uses the MicroBooNE liquid argon time projection chamber to search for decays of these Higgs-portal scalar particles through the Se+e channel with the decays of kaons in the NuMI neutrino beam acting as the source of the scalar particles. The analysis uses an exposure of 2.01×1021 protons on target of NuMI beam data including periods when the beam focusing system was configured to focus positively charged hadrons and separate periods when negatively charged hadrons were focused. The analysis searches for scalar particles produced from kaons decaying in flight in the beam’s decay volume and at rest in the target and absorber. At mS=125MeV (mS=150MeV) we set a limit of θ<3.19×104 (θ<2.79×104) at the 95% confidence level.

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