Measurement of the top-quark pole mass in dileptonic $$ t\overline{t} $$ + 1-jet events at $$ \sqrt{s}=13 $$ TeV with the ATLAS experiment

A bstract A measurement of the top-quark pole mass $$ {m}_t^{\textrm{pole}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>m</mml:mi> <mml:mi>t</mml:mi> <mml:mtext>pole</mml:mtext> </mml:msubsup> </mml:math> is presented in $$ t\overline{t} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> events with an additional jet, $$ t\overline{t} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> + 1-jet, produced in pp collisions at $$ \sqrt{s}=13 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msqrt> <mml:mi>s</mml:mi> </mml:msqrt> <mml:mo>=</mml:mo> <mml:mn>13</mml:mn> </mml:math> TeV. The data sample, recorded with the ATLAS experiment during Run 2 of the LHC, corresponds to an integrated luminosity of 140 fb − 1 . Events with one electron and one muon of opposite electric charge in the final state are selected to measure the $$ t\overline{t} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> + 1-jet differential cross-section as a function of the inverse of the invariant mass of the $$ t\overline{t} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> + 1-jet system. Iterative Bayesian Unfolding is used to correct the data to enable comparison with fixed-order calculations at next-to-leading-order accuracy in the strong coupling. The process $$ pp\to t\overline{t}j\left(2\to 3\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>pp</mml:mi> <mml:mo>→</mml:mo> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>j</mml:mi> <mml:mfenced> <mml:mrow> <mml:mn>2</mml:mn> <mml:mo>→</mml:mo> <mml:mn>3</mml:mn> </mml:mrow> </mml:mfenced> </mml:math> , where top quarks are taken as stable particles, and the process $$ pp\to b\overline{b}{l}^{+}\nu {l}^{-}\overline{\nu}j\left(2\to 7\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>pp</mml:mi> <mml:mo>→</mml:mo> <mml:mi>b</mml:mi> <mml:mover> <mml:mi>b</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:msup> <mml:mi>l</mml:mi> <mml:mo>+</mml:mo> </mml:msup> <mml:mi>ν</mml:mi> <mml:msup> <mml:mi>l</mml:mi> <mml:mo>−</mml:mo> </mml:msup> <mml:mover> <mml:mi>ν</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>j</mml:mi> <mml:mfenced> <mml:mrow> <mml:mn>2</mml:mn> <mml:mo>→</mml:mo> <mml:mn>7</mml:mn> </mml:mrow> </mml:mfenced> </mml:math> , which includes top-quark decays to the dilepton final state and off-shell effects, are considered. The top-quark mass is extracted using a χ 2 fit of the unfolded normalized differential cross-section distribution. The results obtained with the 2 → 3 and 2 → 7 calculations are compatible within theoretical uncertainties, providing an important consistency check. The more precise determination is obtained for the 2 → 3 measurement: $$ {m}_t^{\textrm{pole}}=170.7\pm 0.3\left(\textrm{stat}.\right)\pm 1.4\left(\textrm{syst}.\right)\pm 0.3\left(\textrm{scale}\right)\pm 0.2\left(\textrm{PDF}\oplus {\alpha}_{\textrm{S}}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>m</mml:mi> <mml:mi>t</mml:mi> <mml:mtext>pole</mml:mtext> </mml:msubsup> <mml:mo>=</mml:mo> <mml:mn>170.7</mml:mn> <mml:mo>±</mml:mo> <mml:mn>0.3</mml:mn> <mml:mfenced> <mml:mrow> <mml:mtext>stat</mml:mtext> <mml:mo>.</mml:mo> </mml:mrow> </mml:mfenced> <mml:mo>±</mml:mo> <mml:mn>1.4</mml:mn> <mml:mfenced> <mml:mrow> <mml:mtext>syst</mml:mtext> <mml:mo>.</mml:mo> </mml:mrow> </mml:mfenced> <mml:mo>±</mml:mo> <mml:mn>0.3</mml:mn> <mml:mfenced> <mml:mtext>scale</mml:mtext> </mml:mfenced> <mml:mo>±</mml:mo> <mml:mn>0.2</mml:mn> <mml:mfenced> <mml:mrow> <mml:mi>PDF</mml:mi>

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Journal
Journal of High Energy Physics
Published
2025-12-03
DOI
https://doi.org/10.1007/jhep12(2025)023
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Particle physics theoretical and experimental studies
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article
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article

Measurement of the top-quark pole mass in dileptonic $$ t\overline{t} $$ + 1-jet events at $$ \sqrt{s}=13 $$ TeV with the ATLAS experiment

D. Britzger, A. Mann, G. Unal, A. Zoccoli et al.
Journal of High Energy Physics
Particle physics theoretical and experimental studies
article

Measurement of the top-quark pole mass in dileptonic $$ t\overline{t} $$ + 1-jet events at $$ \sqrt{s}=13 $$ TeV with the ATLAS experiment

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Zhang, G. Carlino, A. G. Rennie, A. A. Talyshev, T. Carli, A. C. Romero Hernandez, N. Lorenzo Martinez, Tim Martin, S. Ali, R. Brener, I. Nikolic-Audit, A. Cortes-Gonzalez, Selim Çetin, C. D. Burgard, N. Semprini-Cesari, B. K. Wosiek, T. Li, C. Wang, J. Han, F. Fabbri, H. J. Yang, D. M. Jones, V. S. Lang, B. Liu, A. Gomes, Y. Chou, T. Yamazaki, S. Kaur, G. Brandt, A. Ghosh, A. Farilla, S. Shimizu, A. G. Borbély, B. R. Roberts, J. Lieber Marin, L. P. Rossi, Л. Н. Смирнова, Elvira Rossi, C. P. Bee, A. S. White, T. Zhao, A. Z. Wang, D. Golubkov, M. J. Fenton, C. L. Cheng, L. Han, H. Wang, A. H. Melo, A. A. Grillo, J. C. Zeng, P. Sherwood, M. Verissimo De Araujo, C. D. Sebastiani, P. Bhattarai, A. D’onofrio, J. Moss, D. Sammel, E. Shabalina, Ruth Pöttgen, N. Hod, S. Hellesund, E. Carquín, E. Bakos, T. J. Stevenson, J. J. Junggeburth, R. Longo, S. Carrá, A. Haas, F. G. Gravili, T. Kharlamova, F. Giuli, S. Ozturk, M. Bosman, B. Eckerova, W. A. Leight, K. Cranmer, D. Derendarz, I. Siral, A. 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article en

Abstract

A bstract A measurement of the top-quark pole mass $$ {m}_t^{\textrm{pole}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>m</mml:mi> <mml:mi>t</mml:mi> <mml:mtext>pole</mml:mtext> </mml:msubsup> </mml:math> is presented in $$ t\overline{t} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> events with an additional jet, $$ t\overline{t} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> + 1-jet, produced in pp collisions at $$ \sqrt{s}=13 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msqrt> <mml:mi>s</mml:mi> </mml:msqrt> <mml:mo>=</mml:mo> <mml:mn>13</mml:mn> </mml:math> TeV. The data sample, recorded with the ATLAS experiment during Run 2 of the LHC, corresponds to an integrated luminosity of 140 fb − 1 . Events with one electron and one muon of opposite electric charge in the final state are selected to measure the $$ t\overline{t} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> + 1-jet differential cross-section as a function of the inverse of the invariant mass of the $$ t\overline{t} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> + 1-jet system. Iterative Bayesian Unfolding is used to correct the data to enable comparison with fixed-order calculations at next-to-leading-order accuracy in the strong coupling. The process $$ pp\to t\overline{t}j\left(2\to 3\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>pp</mml:mi> <mml:mo>→</mml:mo> <mml:mi>t</mml:mi> <mml:mover> <mml:mi>t</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>j</mml:mi> <mml:mfenced> <mml:mrow> <mml:mn>2</mml:mn> <mml:mo>→</mml:mo> <mml:mn>3</mml:mn> </mml:mrow> </mml:mfenced> </mml:math> , where top quarks are taken as stable particles, and the process $$ pp\to b\overline{b}{l}^{+}\nu {l}^{-}\overline{\nu}j\left(2\to 7\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>pp</mml:mi> <mml:mo>→</mml:mo> <mml:mi>b</mml:mi> <mml:mover> <mml:mi>b</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:msup> <mml:mi>l</mml:mi> <mml:mo>+</mml:mo> </mml:msup> <mml:mi>ν</mml:mi> <mml:msup> <mml:mi>l</mml:mi> <mml:mo>−</mml:mo> </mml:msup> <mml:mover> <mml:mi>ν</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>j</mml:mi> <mml:mfenced> <mml:mrow> <mml:mn>2</mml:mn> <mml:mo>→</mml:mo> <mml:mn>7</mml:mn> </mml:mrow> </mml:mfenced> </mml:math> , which includes top-quark decays to the dilepton final state and off-shell effects, are considered. The top-quark mass is extracted using a χ 2 fit of the unfolded normalized differential cross-section distribution. The results obtained with the 2 → 3 and 2 → 7 calculations are compatible within theoretical uncertainties, providing an important consistency check. The more precise determination is obtained for the 2 → 3 measurement: $$ {m}_t^{\textrm{pole}}=170.7\pm 0.3\left(\textrm{stat}.\right)\pm 1.4\left(\textrm{syst}.\right)\pm 0.3\left(\textrm{scale}\right)\pm 0.2\left(\textrm{PDF}\oplus {\alpha}_{\textrm{S}}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>m</mml:mi> <mml:mi>t</mml:mi> <mml:mtext>pole</mml:mtext> </mml:msubsup> <mml:mo>=</mml:mo> <mml:mn>170.7</mml:mn> <mml:mo>±</mml:mo> <mml:mn>0.3</mml:mn> <mml:mfenced> <mml:mrow> <mml:mtext>stat</mml:mtext> <mml:mo>.</mml:mo> </mml:mrow> </mml:mfenced> <mml:mo>±</mml:mo> <mml:mn>1.4</mml:mn> <mml:mfenced> <mml:mrow> <mml:mtext>syst</mml:mtext> <mml:mo>.</mml:mo> </mml:mrow> </mml:mfenced> <mml:mo>±</mml:mo> <mml:mn>0.3</mml:mn> <mml:mfenced> <mml:mtext>scale</mml:mtext> </mml:mfenced> <mml:mo>±</mml:mo> <mml:mn>0.2</mml:mn> <mml:mfenced> <mml:mrow> <mml:mi>PDF</mml:mi>

Journal of High Energy PhysicsVol. 2025(12)
Yeditepe University (TR), Universidade Federal de Juiz de Fora (BR), Northern Illinois University (US), Tbilisi State University (GE), Institut polytechnique de Grenoble (FR), University of Pisa (IT), University of Geneva (CH), University of Rome Tor Vergata (IT), University of Bern (CH), Roma Tre University (IT), Institució Catalana de Recerca i Estudis Avançats (ES), Tufts University (US), Universidade Federal do Rio de Janeiro (BR), Universitat Autònoma de Barcelona (ES), Uppsala University (SE), University of Copenhagen (DK), Universidade Federal da Bahia (BR), University of Iowa (US), Mohammed V University (MA), University of Science and Technology of China (CN), Azerbaijan National Academy of Sciences (AZ), Jagiellonian University (PL), California State University System (US), Argonne National Laboratory (US), Rutherford Appleton Laboratory (GB), University of Udine (IT), Centre National de la Recherche Scientifique (FR), The University of Sydney (AU), A. Alikhanyan National Laboratory (AM), TOBB University of Economics and Technology (TR), Université Toulouse III - Paul Sabatier (FR), Mongolian Academy of Sciences (MN), University of Bonn (DE), Kyushu University (JP), University of Arizona (US), Alexandru Ioan Cuza University (RO), High Energy Accelerator Research Organization (JP), Universidad Andrés Bello (CL), University of Bucharest (RO), University of Lisbon (PT), University of British Columbia (CA), University of Salento (IT), University of Thessaly (GR), Radboud University Nijmegen (NL), University of Tsukuba (JP), University of Liverpool (GB), Lawrence Berkeley National Laboratory (US), Ankara University (TR), Waseda University (JP), Consejo Nacional de Investigaciones Científicas y Técnicas (AR), University of Ljubljana (SI), Shandong University (CN), University of Fribourg (CH), University of Alberta (CA), University of Cape Town (ZA), Sun Yat-sen University (CN), Universität Hamburg (DE), Universitat de València (ES), University of Freiburg (DE), Stockholm University (SE), Pontificia Universidad Católica de Chile (CL), University of Sussex (GB), Tel Aviv University (IL), University of South Africa (ZA), The University of Melbourne (AU), Queen Mary University of London (GB), University of Wuppertal (DE), University of Pittsburgh (US), Duke University (US), Henan University (CN), Iowa State University (US), City University of New York (US), Technion – Israel Institute of Technology (IL), National Technical University of Athens (GR), An-Najah National University (PS), Khalifa University of Science and Technology (AE), Chinese University of Hong Kong (HK), Southern Methodist University (US), Université Fédérale de Toulouse Midi-Pyrénées (FR), Universidade de São Paulo (BR), Simon Fraser University (CA), Ilia State University (GE), Shanghai Jiao Tong University (CN), Parthenope University of Naples (IT), King's College London (GB), Royal Holloway University of London (GB), University of Oslo (NO), University of California, Santa Cruz (US), University of Toronto (CA), University of Tarapacá (CL), Lund University (SE), University of Colorado Boulder (US), University of Milan (IT), The University of Texas at Arlington (US), Universität Innsbruck (AT), York University (CA), University of the Witwatersrand (ZA), University of Trento (IT), Johannes Gutenberg University Mainz (DE), Chinese Academy of Sciences (CN), Université Clermont Auvergne (FR), Millennium Institute (BR), TU Dortmund University (DE), Justus-Liebig-Universität Gießen (DE), Hong Kong University of Science and Technology (HK), National and Kapodistrian University of Athens (GR), Brookhaven National Laboratory (US), University of Washington (US), United Arab Emirates University (AE), National Centre of Scientific Research "Demokritos" (GR), University of California, Irvine (US), Université Paris Cité (FR), University of Siegen (DE), Slovak Academy of Sciences (SK), University of Victoria (CA), Charles University (CZ), Aristotle University of Thessaloniki (GR), Aix-Marseille Université (FR), Kyoto University (JP), Heidelberg University (DE), University of Münster (DE), Hellenic Open University (GR), University of Johannesburg (ZA), University of Cambridge (GB), Universidad de Buenos Aires (AR), Bulgarian Academy of Sciences (BG), Washington College (US), University of Pavia (IT), National Tsing Hua University (TW), University of Würzburg (DE), Stellenbosch University (ZA), Ochanomizu University (JP), Commissariat à l'Énergie Atomique et aux Énergies Alternatives (FR), Université Paris-Saclay (FR), University of Michigan (US), LIP - Laboratory of Instrumentation and Experimental Particle Physics (PT), Folkwang University of the Arts (DE), Harvard University Press (US), Deutsches Elektronen-Synchrotron DESY (DE), University of Illinois System (US), SLAC National Accelerator Laboratory (US), University of California System (US), University of Manchester (GB), University of Sharjah (AE), West University of Timişoara (RO), Université Ibn-Tofail (MA), Transylvania University of Brașov (RO), San Sebastián University (CL), National University of Science and Technology (ZW), Yale University (US), Universidad Nacional de Colombia (CO), California University of Pennsylvania (US), Zhengzhou University (CN), Humboldt-Universität zu Berlin (DE), University of Warwick (GB), Sorbonne Université (FR), Universidade do Estado do Rio de Janeiro (BR), University of Oxford (GB), Islamic University (BD), University of Chicago (US), University of Belgrade (RS), Shanghai Institute for Science of Science (CN), iThemba Laboratory (ZA), Max Planck Institute for Physics (DE), Istituto Nazionale di Fisica Nucleare, Sezione di Roma Tre (IT), Sorbonne Paris Cité (FR), Institute of Experimental Physics of the Slovak Academy of Sciences (SK), Horia Hulubei National Institute for R and D in Physics and Nuclear Engineering (RO), Istituto Nazionale di Fisica Nucleare, Trento Institute for Fundamental Physics And Applications (IT), National Institute for Subatomic Physics (NL), University of West Attica (GR), Istituto Nazionale di Fisica Nucleare, Sezione di Lecce (IT), Institute of Particle Physics (CA), Universidad Antonio Nariño (CO), Instituto de Física Corpuscular (ES), Laboratoire de Physique Nucléaire et de Hautes Énergies (FR), Institute of Nuclear Physics, Polish Academy of Sciences (PL), Istituto Nazionale di Fisica Nucleare, Sezione di Napoli (IT), Istituto Nazionale di Fisica Nucleare, Sezione di Pavia (IT), Instituto de Física La Plata (AR), Istituto Nazionale di Fisica Nucleare, Roma Tor Vergata (IT), Institute for Nuclear Research and Nuclear Energy (BG), The Polytechnic University of Japan (JP), Istinye University (TR), FZU ‒ Institute of Physics of the Academy of Sciences of the Czech Republic (CZ), Istituto Nazionale di Fisica Nucleare, Sezione di Genova (IT), Collaborative Innovation Center of Quantum Matter (CN), CEA Paris-Saclay (FR), Université Mohammed VI Polytechnique (MA), Oklahoma State University Oklahoma City (US), Barcelona Institute of Science and Technology (ES), Institut National de Physique Nucléaire et de Physique des Particules (FR), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (FR), Istituto Nazionale di Fisica Nucleare, Sezione di Milano (IT), Universidad Técnica Federico Santa María (EC), Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali di Frascati (IT), Centro Nacional de Microelectrónica (ES), National Institute for Research and Development of Isotopic and Molecular Technologies (RO), Istituto Nazionale di Fisica Nucleare, Sezione di Bologna (IT), Istituto Nazionale di Fisica Nucleare, Sezione di Trieste (IT), Istituto Nazionale di Fisica Nucleare, Sezione di Roma I (IT), Institut de Microelectrònica de Barcelona (ES), Istituto Nazionale di Fisica Nucleare, Sezione di Pisa (IT), Ōtani University (JP), University of Chinese Academy of Sciences (CN), Institut de Recherche sur les Lois Fondamentales de l'Univers (FR), Instituto de Física de Buenos Aires (AR), Institute of Science and Technology, Istituto Nazionale di Fisica Nucleare, Gruppo Collegato di Udine, Boğaziçi University (TR), University of Bergen (NO), Czech Technical University in Prague (CZ), University College London (GB), University of Calabria (IT), McGill University (CA), The Ohio State University (US), Fundación Ciencias Exactas y Naturales (AR), Weizmann Institute of Science (IL), The University of Adelaide (AU), New York University (US), Sofia University "St. Kliment Ohridski" (BG), Indiana University (US), Stony Brook University (US), Gaziantep University (TR), Nagoya University (JP), Universidad Autónoma de Madrid (ES), Kobe University (JP), Carleton University (CA), European Organization for Nuclear Research (CH), Lancaster University (GB), Istanbul University (TR), AGH University of Krakow (PL), Brandeis University (US), Tokyo Metropolitan University (JP), Palacký University Olomouc (CZ), Université Savoie Mont Blanc (FR), Université de Montréal (CA), University of Göttingen (DE), Comenius University Bratislava (SK), The University of Tokyo (JP), University of La Serena (CL), Premier University (BD), University of Coimbra (PT), Bolu Abant İzzet Baysal University (TR), Columbia University (US), Technische Universität Dresden (DE), University of Glasgow (GB), University of Birmingham (GB), Ludwig-Maximilians-Universität München (DE), University of Genoa (IT), Academia Sinica (TW), Sapienza University of Rome (IT), The University of Texas at Austin (US), University of Oklahoma (US), KTH Royal Institute of Technology (SE), University of the Philippines Diliman (PH), Michigan State University (US), Universidad Nacional de La Plata (AR), Nanjing University (CN), RWTH Aachen University (DE), University of Hong Kong (HK), Universidad Nacional Autónoma de México (MX), Université Grenoble Alpes (FR), University of Sheffield (GB), Louisiana Tech University (US), University of Bologna (IT), Westmont College (US), Stanford University (US), University of Edinburgh (GB), University of the Aegean (GR), Tsinghua University (CN), University of Hassan II Casablanca (MA), University of Minho (PT)
National Science Foundation, U.S. Department of Energy, Alexander von Humboldt-Stiftung, Canarie, Baden-Württemberg Stiftung, CERN, UK Research and Innovation, Centres de Recerca de Catalunya, Türkiye Enerji, Nükleer ve Maden Araştırma Kurumu, Leverhulme Trust, Royal Society, European Commission, Deutsche Forschungsgemeinschaft, Agence Nationale de la Recherche, Ministry of Education, Culture, Sports, Science and Technology, Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung, Danmarks Grundforskningsfond, Fundação de Amparo à Pesquisa do Estado de São Paulo, National Natural Science Foundation of China, Ministerstvo Školství, Mládeže a Tělovýchovy, Grantová Agentura České Republiky, Bundesministerium für Bildung und Forschung, Austrian Science Fund, Generalitat de Catalunya, Ministry of Science and Technology of the People's Republic of China, Nederlandse Organisatie voor Wetenschappelijk Onderzoek, Generalitat Valenciana, Bundesministerium für Wissenschaft, Forschung und Wirtschaft, Conselho Nacional de Desenvolvimento Científico e Tecnológico, Max-Planck-Gesellschaft, Ministerstwo Edukacji i Nauki, Centre National de la Recherche Scientifique, Centre National pour la Recherche Scientifique et Technique, Forskningsrådet om Hälsa, Arbetsliv och Välfärd, Narodowa Agencja Wymiany Akademickiej, Agencia Nacional de Investigación y Desarrollo, National Science and Technology Council, Horizon 2020 Framework Programme, Natural Sciences and Engineering Research Council of Canada, Science and Technology Facilities Council, Japan Society for the Promotion of Science, Fundação para a Ciência e a Tecnologia, Agencia Nacional de Promoción Científica y Tecnológica, British Columbia Knowledge Development Fund, European Regional Development Fund, Agencia Estatal de Investigación, Institut National de Physique Nucléaire et de Physique des Particules, European Social Fund, H2020 European Research Council, H2020 Marie Skłodowska-Curie Actions, CHIST-ERA
Openalex Percentile: Top 82%
Particle physics theoretical and experimental studies
DOIOpen Access PDFOpenAlex
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