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  • Letter
  • Open Access

Enhanced search for neutral current Δ radiative single-photon production in MicroBooNE

P. Abratenko39, D. Andrade Aldana14, L. Arellano22, J. Asaadi38, A. Ashkenazi37, S. Balasubramanian12, B. Baller12, A. Barnard29, G. Barr29 et al. (The MicroBooNE Collaboration*)

G. Barr29, D. Barrow29, J. Barrow26, V. Basque12, J. Bateman15,22, O. Benevides Rodrigues14, S. Berkman25, A. Bhat7, M. Bhattacharya12, M. Bishai3, A. Blake19, B. Bogart24, T. Bolton18, M. B. Brunetti17,41, L. Camilleri10, D. Caratelli4, F. Cavanna12, G. Cerati12, A. Chappell41, Y. Chen33, J. M. Conrad23, M. Convery33, L. Cooper-Troendle30, J. I. Crespo-Anadón6, R. Cross41, M. Del Tutto12, S. R. Dennis5, P. Detje5, R. Diurba2, Z. Djurcic1, K. Duffy29, S. Dytman30, B. Eberly35, P. Englezos32, A. Ereditato7,12, J. J. Evans22, C. Fang4, W. Foreman14,20, B. T. Fleming7, D. Franco7, A. P. Furmanski26, F. Gao4, D. Garcia-Gamez13, S. Gardiner12, G. Ge10, S. Gollapinni20, E. Gramellini22, P. Green29, H. Greenlee12, L. Gu19, W. Gu3, R. Guenette22, P. Guzowski22, L. Hagaman7, M. D. Handley5, O. Hen23, C. Hilgenberg26, G. A. Horton-Smith18, A. Hussain18, B. Irwin26, M. S. Ismail30, C. James12, X. Ji27, J. H. Jo3, R. A. Johnson8, D. Kalra10, G. Karagiorgi10, W. Ketchum12, M. Kirby3, T. Kobilarcik12, N. Lane15,22, J.-Y. Li11, Y. Li3, K. Lin32, B. R. Littlejohn14, L. Liu12, W. C. Louis20, X. Luo4, T. Mahmud19, N. Majeed18, C. Mariani40, D. Marsden22, J. Marshall41, N. Martinez18, D. A. Martinez Caicedo34, S. Martynenko3, A. Mastbaum32, I. Mawby19, N. McConkey31, L. Mellet25, J. Mendez21, J. Micallef23,39, A. Mogan9, T. Mohayai16, M. Mooney9, A. F. Moor5, C. D. Moore12, L. Mora Lepin22, M. M. Moudgalya22, S. Mulleriababu2, D. Naples30, A. Navrer-Agasson15, N. Nayak3, M. Nebot-Guinot11, C. Nguyen32, J. Nowak19, N. Oza10, O. Palamara12, N. Pallat26, V. Paolone30, A. Papadopoulou1, V. Papavassiliou28, H. B. Parkinson11, S. F. Pate28, N. Patel19, Z. Pavlovic12, E. Piasetzky37, K. Pletcher25, I. Pophale19, X. Qian3, J. L. Raaf12, V. Radeka3, A. Rafique1, M. Reggiani-Guzzo11, J. Rodriguez Rondon34, M. Rosenberg39, M. Ross-Lonergan20, I. Safa10, D. W. Schmitz7, A. Schukraft12, W. Seligman10, M. H. Shaevitz10, R. Sharankova12, J. Shi5, E. L. Snider12, M. Soderberg36, S. Söldner-Rembold15, J. Spitz24, M. Stancari12, J. St. John12, T. Strauss12, K. Sutton10, A. M. Szelc11, N. Taniuchi5, K. Terao33, C. Thorpe22, D. Torbunov3, D. Totani4, M. Toups12, A. Trettin22, Y.-T. Tsai33, J. Tyler18, M. A. Uchida5, T. Usher33, B. Viren3, J. Wang27, M. Weber2, H. Wei21, A. J. White7, S. Wolbers12, T. Wongjirad39, K. Wresilo5, W. Wu30, E. Yandel4,20, 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
  • 17The University of Kansas, Lawrence, Kansas 66045, USA
  • 18Kansas State University (KSU), Manhattan, Kansas 66506, USA
  • 19Lancaster University, Lancaster LA1 4YW, United Kingdom
  • 20Los Alamos National Laboratory (LANL), Los Alamos, New Mexico 87545, USA
  • 21Louisiana State University, Baton Rouge, Louisiana 70803, USA
  • 22The University of Manchester, Manchester M13 9PL, United Kingdom
  • 23Massachusetts Institute of Technology (MIT), Cambridge, Massachusetts 02139, USA
  • 24University of Michigan, Ann Arbor, Michigan 48109, USA
  • 25Michigan State University, East Lansing, Michigan 48824, USA
  • 26University of Minnesota, Minneapolis, Minnesota 55455, USA
  • 27Nankai University, Nankai District, Tianjin 300071, China
  • 28New Mexico State University (NMSU), Las Cruces, New Mexico 88003, USA
  • 29University of Oxford, Oxford OX1 3RH, United Kingdom
  • 30University of Pittsburgh, Pittsburgh, Pennsylvania 15260, USA
  • 31Queen Mary University of London, London E1 4NS, United Kingdom
  • 32Rutgers University, Piscataway, New Jersey 08854, USA
  • 33SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
  • 34South Dakota School of Mines and Technology (SDSMT), Rapid City, South Dakota 57701, USA
  • 35University of Southern Maine, Portland, Maine 04104, USA
  • 36Syracuse University, Syracuse, New York 13244, USA
  • 37Tel Aviv University, Tel Aviv, Israel, 69978
  • 38University of Texas, Arlington, Texas 76019, USA
  • 39Tufts University, Medford, Massachusetts 02155, USA
  • 40Center for Neutrino Physics, Virginia Tech, Blacksburg, Virginia 24061, USA
  • 41University of Warwick, Coventry CV4 7AL, United Kingdom

  • *Contact author: microboone_info@fnal.gov

Phys. Rev. D 112, L091101 – Published 17 November, 2025

DOI: https://doi.org/10.1103/49ds-5hfh

Abstract

We report results from an updated search for neutral current (NC) resonant Δ(1232) baryon production and subsequent Δ radiative decay (NC Δ→Nγ). We consider events with and without final state protons; events with a proton can be compared with the kinematics of a Δ(1232) baryon decay, while events without a visible proton represent a more generic phase space. In order to maximize sensitivity to each topology, we simultaneously make use of two different reconstruction paradigms, Pandora and Wire-Cell, which have complementary strengths, and select mostly orthogonal sets of events. Considering an overall scaling of the NC Δ→Nγ rate as an explanation of the MiniBooNE anomaly, our data exclude this hypothesis at 94.4% CL. When we decouple the expected correlations between NC Δ→Nγ events with and without final state protons, our data exclude an interpretation in which all excess events have associated protons at 2.0σ, and are consistent with an interpretation in which all excess events have no associated protons at 0.63σ.

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