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Feasibility studies for the measurement of time-like proton electromagnetic form factors from p¯ p→ μ+μ- at P ¯ ANDA at FAIR. / The PANDA Collaboration; Блинов, Александр Евгеньевич; Кравченко, Евгений Анатольевич.

In: European Physical Journal A, Vol. 57, No. 1, 30, 01.2021.

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The PANDA Collaboration, Блинов АЕ, Кравченко ЕА. Feasibility studies for the measurement of time-like proton electromagnetic form factors from p¯ p→ μ+μ- at P ¯ ANDA at FAIR. European Physical Journal A. 2021 Jan;57(1):30. doi: 10.1140/epja/s10050-020-00333-3

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The PANDA Collaboration ; Блинов, Александр Евгеньевич ; Кравченко, Евгений Анатольевич. / Feasibility studies for the measurement of time-like proton electromagnetic form factors from p¯ p→ μ+μ- at P ¯ ANDA at FAIR. In: European Physical Journal A. 2021 ; Vol. 57, No. 1.

BibTeX

@article{7b6becf76bd04f52bbaa5845ae704247,
title = "Feasibility studies for the measurement of time-like proton electromagnetic form factors from p¯ p→ μ+μ- at P ¯ ANDA at FAIR",
abstract = "This paper reports on Monte Carlo simulation results for future measurements of the moduli of time-like proton electromagnetic form factors, | GE| and | GM| , using the p¯ p→ μ+μ- reaction at P ¯ ANDA (FAIR). The electromagnetic form factors are fundamental quantities parameterizing the electric and magnetic structure of hadrons. This work estimates the statistical and total accuracy with which the form factors can be measured at P ¯ ANDA , using an analysis of simulated data within the PandaRoot software framework. The most crucial background channel is p¯ p→ π+π-, due to the very similar behavior of muons and pions in the detector. The suppression factors are evaluated for this and all other relevant background channels at different values of antiproton beam momentum. The signal/background separation is based on a multivariate analysis, using the Boosted Decision Trees method. An expected background subtraction is included in this study, based on realistic angular distributions of the background contribution. Systematic uncertainties are considered and the relative total uncertainties of the form factor measurements are presented.",
author = "{The PANDA Collaboration} and G. Barucca and F. Dav{\`i} and G. Lancioni and P. Mengucci and L. Montalto and Natali, {P. P.} and N. Paone and D. Rinaldi and L. Scalise and W. Erni and B. Krusche and M. Steinacher and N. Walford and N. Cao and Z. Liu and C. Liu and B. Liu and X. Shen and S. Sun and J. Tao and Xiong, {X. A.} and G. Zhao and J. Zhao and M. Albrecht and W. Alkakhi and S. B{\"o}kelmann and S. Coen and F. Feldbauer and M. Fink and J. Frech and V. Freudenreich and M. Fritsch and J. Grochowski and R. Hagdorn and Heinsius, {F. H.} and T. Held and T. Holtmann and I. Keshk and H. Koch and B. Kopf and M. Kuhlmann and M. K{\"u}mmel and M. K{\"u}{\ss}ner and J. Li and L. Linzen and S. Kononov and Barnyakov, {A. Yu} and K. Beloborodov and Kuyanov, {I. A.} and S. Pivovarov and Блинов, {Александр Евгеньевич} and Кравченко, {Евгений Анатольевич}",
note = "Funding Information: We acknowledge financial support from the Science and Technology Facilities Council (STFC), British funding agency, Great Britain; the Bhabha Atomic Research Centre (BARC) and the Indian Institute of Technology Bombay, India; the Bundesministerium f{\"u}r Bildung und Forschung (BMBF), Germany; the Carl-Zeiss-Stiftung 21-0563-2.8/122/1 and 21-0563-2.8/131/1, Mainz, Germany; the Center for Advanced Radiation Technology (KVI-CART), Groningen, Netherlands; the CNRS/IN2P3 and the Universit{\'e} Paris-Sud, France; the Czech Ministry (MEYS) Grants LM2015049, CZ.02.1.01/0.0/0.0/16 and 013/0001677, the Deutsche Forschungsgemeinschaft (DFG), Germany; the Deutscher Akademischer Austauschdienst (DAAD), Germany; the Forschungszentrum J{\"u}lich, Germany; the European Union{\textquoteright}s Horizon 2020 research and innovation program under grant agreement No 824093; the Gesellschaft f{\"u}r Schwerionenforschung GmbH (GSI), Darmstadt, Germany; the Helmholtz-Gemeinschaft Deutscher Forschungszentren (HGF), Germany; the INTAS, European Commission funding; the Institute of High Energy Physics (IHEP) and the Chinese Academy of Sciences, Beijing, China; the Istituto Nazionale di Fisica Nucleare (INFN), Italy; the Ministerio de Educacion y Ciencia (MEC) under Grant FPA2006-12120-C03-02; the Polish Ministry of Science and Higher Education (MNiSW) Grant No. 2593/7, PR UE/2012/2, and the National Science Centre (NCN) DEC-2013/09/N/ST2/02180, Poland; the State Atomic Energy Corporation Rosatom, National Research Center Kurchatov Institute, Russia; the Schweizerischer Nationalfonds zur F{\"o}rderung der Wissenschaftlichen Forschung (SNF), Swiss; the Stefan Meyer Institut f{\"u}r Subatomare Physik and the {\"O}sterreichische Akademie der Wissenschaften, Wien, Austria; the Swedish Research Council and the Knut and Alice Wallenberg Foundation, Sweden; the Scientific and Technological Research Council of Turkey (TUBITAK) under Grant No. 119F094. Publisher Copyright: {\textcopyright} 2021, The Author(s). Copyright: Copyright 2021 Elsevier B.V., All rights reserved.",
year = "2021",
month = jan,
doi = "10.1140/epja/s10050-020-00333-3",
language = "English",
volume = "57",
journal = "European Physical Journal A",
issn = "1434-6001",
publisher = "Springer Nature",
number = "1",

}

RIS

TY - JOUR

T1 - Feasibility studies for the measurement of time-like proton electromagnetic form factors from p¯ p→ μ+μ- at P ¯ ANDA at FAIR

AU - The PANDA Collaboration

AU - Barucca, G.

AU - Davì, F.

AU - Lancioni, G.

AU - Mengucci, P.

AU - Montalto, L.

AU - Natali, P. P.

AU - Paone, N.

AU - Rinaldi, D.

AU - Scalise, L.

AU - Erni, W.

AU - Krusche, B.

AU - Steinacher, M.

AU - Walford, N.

AU - Cao, N.

AU - Liu, Z.

AU - Liu, C.

AU - Liu, B.

AU - Shen, X.

AU - Sun, S.

AU - Tao, J.

AU - Xiong, X. A.

AU - Zhao, G.

AU - Zhao, J.

AU - Albrecht, M.

AU - Alkakhi, W.

AU - Bökelmann, S.

AU - Coen, S.

AU - Feldbauer, F.

AU - Fink, M.

AU - Frech, J.

AU - Freudenreich, V.

AU - Fritsch, M.

AU - Grochowski, J.

AU - Hagdorn, R.

AU - Heinsius, F. H.

AU - Held, T.

AU - Holtmann, T.

AU - Keshk, I.

AU - Koch, H.

AU - Kopf, B.

AU - Kuhlmann, M.

AU - Kümmel, M.

AU - Küßner, M.

AU - Li, J.

AU - Linzen, L.

AU - Kononov, S.

AU - Barnyakov, A. Yu

AU - Beloborodov, K.

AU - Kuyanov, I. A.

AU - Pivovarov, S.

AU - Блинов, Александр Евгеньевич

AU - Кравченко, Евгений Анатольевич

N1 - Funding Information: We acknowledge financial support from the Science and Technology Facilities Council (STFC), British funding agency, Great Britain; the Bhabha Atomic Research Centre (BARC) and the Indian Institute of Technology Bombay, India; the Bundesministerium für Bildung und Forschung (BMBF), Germany; the Carl-Zeiss-Stiftung 21-0563-2.8/122/1 and 21-0563-2.8/131/1, Mainz, Germany; the Center for Advanced Radiation Technology (KVI-CART), Groningen, Netherlands; the CNRS/IN2P3 and the Université Paris-Sud, France; the Czech Ministry (MEYS) Grants LM2015049, CZ.02.1.01/0.0/0.0/16 and 013/0001677, the Deutsche Forschungsgemeinschaft (DFG), Germany; the Deutscher Akademischer Austauschdienst (DAAD), Germany; the Forschungszentrum Jülich, Germany; the European Union’s Horizon 2020 research and innovation program under grant agreement No 824093; the Gesellschaft für Schwerionenforschung GmbH (GSI), Darmstadt, Germany; the Helmholtz-Gemeinschaft Deutscher Forschungszentren (HGF), Germany; the INTAS, European Commission funding; the Institute of High Energy Physics (IHEP) and the Chinese Academy of Sciences, Beijing, China; the Istituto Nazionale di Fisica Nucleare (INFN), Italy; the Ministerio de Educacion y Ciencia (MEC) under Grant FPA2006-12120-C03-02; the Polish Ministry of Science and Higher Education (MNiSW) Grant No. 2593/7, PR UE/2012/2, and the National Science Centre (NCN) DEC-2013/09/N/ST2/02180, Poland; the State Atomic Energy Corporation Rosatom, National Research Center Kurchatov Institute, Russia; the Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung (SNF), Swiss; the Stefan Meyer Institut für Subatomare Physik and the Österreichische Akademie der Wissenschaften, Wien, Austria; the Swedish Research Council and the Knut and Alice Wallenberg Foundation, Sweden; the Scientific and Technological Research Council of Turkey (TUBITAK) under Grant No. 119F094. Publisher Copyright: © 2021, The Author(s). Copyright: Copyright 2021 Elsevier B.V., All rights reserved.

PY - 2021/1

Y1 - 2021/1

N2 - This paper reports on Monte Carlo simulation results for future measurements of the moduli of time-like proton electromagnetic form factors, | GE| and | GM| , using the p¯ p→ μ+μ- reaction at P ¯ ANDA (FAIR). The electromagnetic form factors are fundamental quantities parameterizing the electric and magnetic structure of hadrons. This work estimates the statistical and total accuracy with which the form factors can be measured at P ¯ ANDA , using an analysis of simulated data within the PandaRoot software framework. The most crucial background channel is p¯ p→ π+π-, due to the very similar behavior of muons and pions in the detector. The suppression factors are evaluated for this and all other relevant background channels at different values of antiproton beam momentum. The signal/background separation is based on a multivariate analysis, using the Boosted Decision Trees method. An expected background subtraction is included in this study, based on realistic angular distributions of the background contribution. Systematic uncertainties are considered and the relative total uncertainties of the form factor measurements are presented.

AB - This paper reports on Monte Carlo simulation results for future measurements of the moduli of time-like proton electromagnetic form factors, | GE| and | GM| , using the p¯ p→ μ+μ- reaction at P ¯ ANDA (FAIR). The electromagnetic form factors are fundamental quantities parameterizing the electric and magnetic structure of hadrons. This work estimates the statistical and total accuracy with which the form factors can be measured at P ¯ ANDA , using an analysis of simulated data within the PandaRoot software framework. The most crucial background channel is p¯ p→ π+π-, due to the very similar behavior of muons and pions in the detector. The suppression factors are evaluated for this and all other relevant background channels at different values of antiproton beam momentum. The signal/background separation is based on a multivariate analysis, using the Boosted Decision Trees method. An expected background subtraction is included in this study, based on realistic angular distributions of the background contribution. Systematic uncertainties are considered and the relative total uncertainties of the form factor measurements are presented.

UR - http://www.scopus.com/inward/record.url?scp=85100155048&partnerID=8YFLogxK

UR - https://www.mendeley.com/catalogue/1a296b49-9ff9-35c3-89cf-38e07a81d549/

U2 - 10.1140/epja/s10050-020-00333-3

DO - 10.1140/epja/s10050-020-00333-3

M3 - Article

AN - SCOPUS:85100155048

VL - 57

JO - European Physical Journal A

JF - European Physical Journal A

SN - 1434-6001

IS - 1

M1 - 30

ER -

ID: 27710785