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Unbinned deep learning jet substructure measurement in high Q2 ep collisions at HERA

  • V. Andreev
  • , M. Arratia
  • , A. Baghdasaryan
  • , A. Baty
  • , K. Begzsuren
  • , A. Bolz
  • , V. Boudry
  • , G. Brandt
  • , D. Britzger
  • , A. Buniatyan
  • , L. Bystritskaya
  • , A. J. Campbell
  • , K. B. Cantun Avila
  • , K. Cerny
  • , V. Chekelian
  • , Z. Chen
  • , J. G. Contreras
  • , J. Cvach
  • , J. B. Dainton
  • , K. Daum
  • A. Deshpande, C. Diaconu, A. Drees, G. Eckerlin, S. Egli, E. Elsen, L. Favart, A. Fedotov, J. Feltesse, M. Fleischer, A. Fomenko, C. Gal, J. Gayler, L. Goerlich, N. Gogitidze, M. Gouzevitch, C. Grab, T. Greenshaw, G. Grindhammer, D. Haidt, R. C.W. Henderson, J. Hessler, J. Hladký, D. Hoffmann, R. Horisberger, T. Hreus, F. Huber, P. M. Jacobs, M. Jacquet, T. Janssen, A. W. Jung, J. Katzy, C. Kiesling, M. Klein, C. Kleinwort, H. T. Klest, R. Kogler, P. Kostka, J. Kretzschmar, D. Krücker, K. Krüger, M. P.J. Landon, W. Lange, P. Laycock, S. H. Lee, S. Levonian, W. Li, J. Lin, K. Lipka, B. List, J. List, B. Lobodzinski, O. R. Long, E. Malinovski, H. U. Martyn, S. J. Maxfield, A. Mehta, A. B. Meyer, J. Meyer, S. Mikocki, V. M. Mikuni, M. M. Mondal, K. Müller, B. Nachman, Th Naumann, P. R. Newman, C. Niebuhr, G. Nowak, J. E. Olsson, D. Ozerov, S. Park, C. Pascaud, G. D. Patel, E. Perez, A. Petrukhin, I. Picuric, D. Pitzl, R. Polifka, S. Preins, V. Radescu, N. Raicevic, T. Ravdandorj, P. Reimer, E. Rizvi, P. Robmann, R. Roosen, A. Rostovtsev, M. Rotaru, D. P.C. Sankey, M. Sauter, E. Sauvan, S. Schmitt, B. A. Schmookler, G. Schnell, L. Schoeffel, A. Schöning, F. Sefkow, S. Shushkevich, Y. Soloviev, P. Sopicki, D. South, A. Specka, M. Steder, B. Stella, U. Straumann, C. Sun, T. Sykora, P. D. Thompson, F. Torales Acosta, D. Traynor, B. Tseepeldorj, Z. Tu, G. Tustin, A. Valkárová, C. Vallée, P. Van Mechelen, D. Wegener, E. Wünsch, J. Žáček, J. Zhang, Z. Zhang, R. Žlebčík, H. Zohrabyan, F. Zomer
  • German Electron Synchrotron
  • University of California at Riverside
  • A. Alikhanian Yerevan Institute of Physics
  • Rice University
  • Mongolian Academy of Sciences
  • Laboratoire Leprince-Ringuet
  • University of Göttingen
  • Max Planck Institute for Physics (Werner Heisenberg Institute)
  • University of Birmingham
  • Centro de Investigacion y de Estudios Avanzados del Instituto Politécnico Nacional
  • Joint Laboratory of Optics
  • Shandong University
  • Czech Academy of Sciences
  • University of Liverpool
  • University of Wuppertal
  • Aix-Marseille Université
  • Paul Scherrer Institute
  • Inter-University Institute for High Energies (ULB-VUB)
  • Université Paris-Saclay
  • Stony Brook University
  • Institute of Nuclear Physics
  • ETH Zurich
  • Lancaster University
  • University of Zurich
  • Heidelberg University 
  • Lawrence Berkeley National Laboratory
  • Purdue University
  • Queen Mary University of London
  • Brookhaven National Laboratory
  • University of Michigan, Ann Arbor
  • RWTH Aachen University
  • CERN
  • University of Siegen
  • University of Montenegro
  • Charles University
  • Horia Hulubei National Institute of Physics and Nuclear Engineering
  • STFC Rutherford Appleton Laboratory (RAL)
  • Université Savoie Mont Blanc
  • University of the Basque Country
  • Roma Tre University
  • National University of Mongolia
  • TU Dortmund University

Research output: Contribution to journalArticlepeer-review

20 Scopus citations

Abstract

The radiation pattern within high energy quark- and gluon-initiated jets (jet substructure) is used extensively as a precision probe of the strong force as well as an environment for optimizing event generators with numerous applications in high energy particle and nuclear physics. Looking at electron-proton collisions is of particular interest as many of the complications present at hadron colliders are absent. A detailed study of modern jet substructure observables, jet angularities, in electron-proton collisions is presented using data recorded using the H1 detector at HERA. The measurement is unbinned and multi-dimensional, using machine learning to correct for detector effects. All of the available reconstructed object information of the respective jets is interpreted by a graph neural network, achieving superior precision on a selected set of jet angularities. Training these networks was enabled by the use of a large number of GPUs in the Perlmutter supercomputer at Berkeley Lab. The particle jets are reconstructed in the laboratory frame, using the kT jet clustering algorithm. Results are reported at high transverse momentum transfer Q2>150GeV2, and inelasticity 0.2<y<0.7. The analysis is also performed in sub-regions of Q2, thus probing scale dependencies of the substructure variables. The data are compared with a variety of predictions and point towards possible improvements of such models.

Original languageEnglish
Article number138101
JournalPhysics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
Volume844
DOIs
StatePublished - Sep 10 2023

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