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Determining the gluonic gravitational form factors of the proton.
Duran, B; Meziani, Z-E; Joosten, S; Jones, M K; Prasad, S; Peng, C; Armstrong, W; Atac, H; Chudakov, E; Bhatt, H; Bhetuwal, D; Boer, M; Camsonne, A; Chen, J-P; Dalton, M M; Deokar, N; Diefenthaler, M; Dunne, J; El Fassi, L; Fuchey, E; Gao, H; Gaskell, D; Hansen, O; Hauenstein, F; Higinbotham, D; Jia, S; Karki, A; Keppel, C; King, P; Ko, H S; Li, X; Li, R; Mack, D; Malace, S; McCaughan, M; McClellan, R E; Michaels, R; Meekins, D; Paolone, Michael; Pentchev, L; Pooser, E; Puckett, A; Radloff, R; Rehfuss, M; Reimer, P E; Riordan, S; Sawatzky, B; Smith, A; Sparveris, N; Szumila-Vance, H.
Afiliação
  • Duran B; Physics Division, Argonne National Laboratory, Lemont, IL, USA.
  • Meziani ZE; Department of Physics, Temple University, Philadelphia, PA, USA.
  • Joosten S; Physics Division, Argonne National Laboratory, Lemont, IL, USA. zmeziani@anl.gov.
  • Jones MK; Department of Physics, Temple University, Philadelphia, PA, USA. zmeziani@anl.gov.
  • Prasad S; Physics Division, Argonne National Laboratory, Lemont, IL, USA.
  • Peng C; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Armstrong W; Physics Division, Argonne National Laboratory, Lemont, IL, USA.
  • Atac H; Physics Division, Argonne National Laboratory, Lemont, IL, USA.
  • Chudakov E; Physics Division, Argonne National Laboratory, Lemont, IL, USA.
  • Bhatt H; Department of Physics, Temple University, Philadelphia, PA, USA.
  • Bhetuwal D; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Boer M; Department of Physics & Astronomy, Mississippi State University, Mississippi State, MS, USA.
  • Camsonne A; Department of Physics & Astronomy, Mississippi State University, Mississippi State, MS, USA.
  • Chen JP; Department of Physics, Virginia Polytechnic Institute & State University, Blacksburg, VA, USA.
  • Dalton MM; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Deokar N; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Diefenthaler M; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Dunne J; Department of Physics, Temple University, Philadelphia, PA, USA.
  • El Fassi L; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Fuchey E; Department of Physics & Astronomy, Mississippi State University, Mississippi State, MS, USA.
  • Gao H; Department of Physics & Astronomy, Mississippi State University, Mississippi State, MS, USA.
  • Gaskell D; Department of Physics, University of Connecticut, Storrs, CT, USA.
  • Hansen O; Department of Physics, Duke University, Durham, NC, USA.
  • Hauenstein F; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Higinbotham D; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Jia S; Department of Physics, Old Dominion University, Norfolk, VA, USA.
  • Karki A; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Keppel C; Department of Physics, Temple University, Philadelphia, PA, USA.
  • King P; Department of Physics & Astronomy, Mississippi State University, Mississippi State, MS, USA.
  • Ko HS; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Li X; Department of Physics and Astronomy, Ohio University, Athens, OH, USA.
  • Li R; CNRS/IN2P3, IJCLab Orsay, Université Paris-Saclay, Gif-sur-Yvette, France.
  • Mack D; Department of Physics, Duke University, Durham, NC, USA.
  • Malace S; Department of Physics, Temple University, Philadelphia, PA, USA.
  • McCaughan M; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • McClellan RE; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Michaels R; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Meekins D; Natural Sciences Department, Pensacola State College, Pensacola, FL, USA.
  • Paolone M; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Pentchev L; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Pooser E; Department of Physics, Temple University, Philadelphia, PA, USA.
  • Puckett A; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Radloff R; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Rehfuss M; Department of Physics, University of Connecticut, Storrs, CT, USA.
  • Reimer PE; Department of Physics and Astronomy, Ohio University, Athens, OH, USA.
  • Riordan S; Department of Physics, Temple University, Philadelphia, PA, USA.
  • Sawatzky B; Physics Division, Argonne National Laboratory, Lemont, IL, USA.
  • Smith A; Physics Division, Argonne National Laboratory, Lemont, IL, USA.
  • Sparveris N; Experimental Nuclear Physics Division, Thomas Jefferson National Accelerator Facility, Newport News, VA, USA.
  • Szumila-Vance H; Department of Physics, Duke University, Durham, NC, USA.
Nature ; 615(7954): 813-816, 2023 03.
Article em En | MEDLINE | ID: mdl-36991189
ABSTRACT
The proton is one of the main building blocks of all visible matter in the Universe1. Among its intrinsic properties are its electric charge, mass and spin2. These properties emerge from the complex dynamics of its fundamental constituents-quarks and gluons-described by the theory of quantum chromodynamics3-5. The electric charge and spin of protons, which are shared among the quarks, have been investigated previously using electron scattering2. An example is the highly precise measurement of the electric charge radius of the proton6. By contrast, little is known about the inner mass density of the proton, which is dominated by the energy carried by gluons. Gluons are hard to access using electron scattering because they do not carry an electromagnetic charge. Here we investigated the gravitational density of gluons using a small colour dipole, through the threshold photoproduction of the J/ψ particle. We determined the gluonic gravitational form factors of the proton7,8 from our measurement. We used a variety of models9-11 and determined, in all cases, a mass radius that is notably smaller than the electric charge radius. In some, but not all cases, depending on the model, the determined radius agrees well with first-principle predictions from lattice quantum chromodynamics12. This work paves the way for a deeper understanding of the salient role of gluons in providing gravitational mass to visible matter.

Texto completo: 1 Base de dados: MEDLINE Tipo de estudo: Prognostic_studies Idioma: En Revista: Nature Ano de publicação: 2023 Tipo de documento: Article País de afiliação: Estados Unidos

Texto completo: 1 Base de dados: MEDLINE Tipo de estudo: Prognostic_studies Idioma: En Revista: Nature Ano de publicação: 2023 Tipo de documento: Article País de afiliação: Estados Unidos