Feasibility studies of time-like proton electromagnetic form factors at $\overline{\rm P}$ P ¯ ANDA at FAIR

Singh, B. P.; Erni, W.; Krusche, B.; Steinacher, M.; Walford, N. K.; Liu, B.; Liu, H.; Liu, Z.; Shen, X. Y.; Wang, C.; Zhao, J.; Albrecht, M.; Erlen, T.; Fink, Martin; Heinsius, F. H.; Held, T.; Holtmann, T.; Jasper, Sarah; Keshk, I. K.; Koch, H.; Kopf, B.; Kuhlmann, M.; Kümmel, M.; Leiber, S.; Mikirtychyants, M.; Musiol, P.; Mustafa, A.; Pelizäus, M.; Pychy, J.; Richter, Markus; Schnier, C.; Schröder, T.; Sowa, C.; Steinke, M.; Triffterer, T.; Wiedner, U.; Ball, M.; Beck, R.; Hammann, Ch.; Ketzer, B.; Kube, M.; Mahlberg, P.; Roßbach, M.; Schmidt, Ch.; Schmitz, R.; Thoma, U.; Urban, M.; Walther, Dirk; Wendel, Ch.; Wilson, A.; Bianconi, A.; Bragadireanu, M.; Caprini, M.; Pantea, D.; Patel, Bhavin; Czyżycki, Wojciech; Domagała, Mariusz; Filo, Grzegorz; Jaworowski, J.; Krawczyk, Maria; Lisowski, Filip; Lisowski, E.; Michałek, M.; Poznański, Piotr; Płażek, J.; Korcyl, K.; Kozela, A.; Kulessa, P.; Lebiedowicz, Piotr; Pysz, K.; Schäfer, Wolfgang; Szczurek, Antoni; Fiutowski, T.; Idzik, M.; Mindur, B.; Przyborowski, D.; Świentek, K.; Biernat, J.; Kamys, B.; Kistryn, S.; Korcyl, G.; Krzemień, W.; Magiera, A.; Moskal, P.; Pyszniak, A.; Rudy, Z.; Salabura, P.; Smyrski, J.; Strzempek, P.; Wrońska, A.; Augustin, I.; Böhm, R.; Lehmann, I.; Marinescu, D. Nicmorus; Schmitt, L.; Varentsov, V.; Al-Turany, M.; Belias, A.; Deppe, H.; Dzhygadlo, R.; Ehret, A.; Flemming, H.; Gerhardt, A.; Götzen, K.; Gromliuk, A.; Gruber, L.; Karabowicz, R.; Kliemt, R.; Krebs, M.; Kurilla, U.; Lehmann, D.; Löchner, S.; Lühning, J.; Lynen, U.; Orth, H.; Patsyuk, M.; Peters, K.; Saito, Takayuki; Schepers, G.; Schmidt, C. J.; Schwarz, C.; Schwiening, J.; Täschner, A.; Traxler, M.; Ugur, C.; Voss, B.; Wieczorek, P.; Wilms, A.; Zühlsdorf, M.; Abazov, V. M.; Alexeev, G. D.; Arefiev, V.; Astakhov, V.; Barabanov, M. Yu.; Batyunya, B.; Davydov, Yu. I.; Dodokhov, V.Kh.; Ефремов, А. В.; Fechtchenko, A.; Fedunov, A.; Galoyan, A.; Grigoryan, S.; Koshurnikov, E. K.; Lobanov, Yu. Yu.; Lobanov, V.I.; Makarov, A.F.; Malinina, L.; Malyshev, V. L.; Olshevskiy, A.; Perevalova, E.; Piskun, A. A.; Pocheptsov, T.; Pontecorvo, G. B.; Rodionov, V. K.; Rogov, Yu. N.; Salmin, R. A.; Samartsev, A.; Sapozhnikov, M. G.; Shabratova, G.; Skachkov, N. B.; Skachkova, A. N.; Strokovsky, E. A.; Suleimanov, M.K.; Тешев, Р. Ш.; Tokmenin, V. V.; Uzhinsky, V.; Vodopianov, A.; Zaporozhets, S.; Zhuravlev, N.; Zorin, A. G.; Branford, D.; Glazier, D. I.; Watts, D. P.; Böhm, Michael; Britting, A.; Eyrich, W.; Lehmann, A.; Pfaffinger, M.; Uhlig, F.; Dobbs, S.; Seth, K. K.; Tomaradze, A.; Xiao, Ting; Bettoni, D.; Carassiti, V.; Ramusino, A. Cotta; Dalpiaz, P.; Drago, A.; Fioravanti, E.; Garzia, I.; Savrié, M.; Akishina, V.; Kisel, I.; Kozlov, G.; Pugach, Megan K.; Zyzak, M.; Gianotti, P.; Guaraldo, C.; Lucherini, V.; Bersani, A.; Bracco, G.; Macrı́, M.; Parodi, R.; Biguenko, K.; Brinkmann, Kai-Thomas; Pietro, V. Di; Diehl, Stefan; Dormenev, V.; Drexler, P.; Düren, M.; Etzelmüller, E.; Galuska, Martin; Gutz, E.; Hahn, C.; Hayrapetyan, A.; Kesselkaul, M.; Kühn, W.; Kuske, Till; Lange, J. S.; Liang, Y. T.; Metag, V.; Nanova, M.; Nazarenko, S.; Novotny, R.; Quagli, T.; Reiter, S.; Rieke, J.; Rosenbaum, Christoph; Schmidt, M.; Schnell, R.; Stenzel, H.; Thöring, U.; Ullrich, M.; Wagner, M. N.; Wasem, T.; Wohlfahrt, B.; Zaunick, Hans-Georg; Ireland, D. G.; Rosner, G.; Seitz, B.; Deepak, P. N.; Kulkarni, A.; Apostolou, A.; Babai, M.; Kavatsyuk, M.; Lemmens, Peter; Lindemulder, M.; Loehner, H.; Messchendorp, J. G.; Schakel, P.; Smit, H.; Tiemens, M.; Weele, J. C. van der; Veenstra, R.; Vejdani, S.; Dutta, K.; Kalita, K.; Kumar, Ajay; Roy, A.; Sohlbach, H.; Bai, Mei; Bianchi, Ludovico; Büscher, M.; Cao, L.; Cebulla, A.; Dosdall, R.; Gillitzer, A.; Goldenbaum, F.; Grunwald, Dirk; Herten, Andreas; Hu, Q.; Kemmerling, G.; Kleines, H.; Lehrach, A.; Nellen, R.; Ohm, H.; Orfanitski, S.; Prasuhn, D.; Prencipe, E.; Pütz, J.; Ritman, J.; Schadmand, S.; Sefzick, T.; Serdyuk, V.; Sterzenbach, G.; Stockmanns, T.; Wintz, P.; Wüstner, P.; Xu, H.; Zambanini, André; Li, S.; Li, Z.; Sun, Zhigang; Rigato, V.; Isaksson, L.; Achenbach, P.; Corell, O.; Denig, A.; Distler, M. O.; Hoek, M.; Karavdina, A.; Lauth, W.; Merkel, H.; Müller, U.; Pochodzalla, J.; Sánchez, S. F.; Schlimme, S.; Sfienti, C.; Thiel, M.; Ahmadi, Hamed; Ahmed, S.; Bleser, S.; Capozza, L.; Cardinali, M.; Dbeyssi, A.; Deiseroth, M.; Feldbauer, F.; Fritsch, M.; Fröhlich, B.; Jasinski, P.; Kang, D. Y.; Khaneft, D.; Klasen, R.; Leithoff, H.; Lin, D. X.; Maas, F. E.; Maldaner, S.; Martínez, M. Lucio; Michel, Martin C.; Espí, M. C. Mora; Morales, C. Morales; Motzko, C.; Nerling, F.; Noll, O.; Pflüger, S.; Pitka, A.; Piñeiro, D. Rodríguez; Lorente, A. Sánchez; Steinen, Marcell; Valente, Riccardo; Weber, T.; Zambrana, M.; Zimmermann, I.; Fedorov, A.; Korjik, M.; Missevitch, O.; Boukharov, A.; Malyshev, O. N.; Marishev, I.; Balanutsa, V.; Balanutsa, P.; Chernetsky, V.; Demekhin, A.; Dolgolenko, A.; Fedorets, P.; Герасимов, А. С.; Goryachev, V.; Chandratre, V.B.; Datar, V. M.; Dutta, D.; Jha, V.; Kumawat, H.; Mohanty, A. K.; Parmar, A.; Roy, B. J.; Sonika, G.; Fritzsch, C.; Grieser, S.; Hergemöller, A. K.; Hetz, B.; Hüsken, N.; Khoukaz, A.; Wessels, J. P.; Khosonthongkee, K.; Kobdaj, C.; Limphirat, A.; Srisawad, Pornrad; Yan, Yupeng; Barnyakov, M.Yu.; Barnyakov, A.; Beloborodov, K.; Blinov, A. E.; Blinov, V.; Bobrovnikov, V. S.; Kononov, S.A.; Kravchenko, E. A.; Kuyanov, I. A.; Martin, K. A.; Onuchin, A. P.; Serednyakov, S. I.; Sokolov, A.; Tikhonov, Yu. A.; Atomssa, E. T.; Kunne, R.; Marchand, D.; Ramstein, B.; Wiele, J. Van de; Wang, Y.; Boca, G.; Costanza, S.; Genova, P.; Montagna, P.; Rotondi, A.; Abramov, V.; Belikov, N.I.; Bukreeva, S.; Davidenko, A. M.; Derevschikov, A. A.; Goncharenko, Y.; Grishin, V.; Качанов, В.; Kormilitsin, V.; Levin, Andrew; Mel'nik, Yu.M.; Minaev, N. G.; Mochalov, V. V.; Морозов, Д. А.; Nogach, L. V.; Poslavskiy, S.; Ryazantsev, A.; Ryzhikov, S.; Semenov, P. A.; Shein, I.; Uzunian, A.; Vasiliev, A. N.; Yakutin, A. E.; Tomasi–Gustafsson, E.; Roy, Utpal; Yabsley, B.; Belostotski, S.; Gavrilov, G.; Izotov, A.; Manaenkov, S. I.; Miklukho, O. V.; Veretennikov, D.; Zhdanov, A. A.; Makónyi, K.; Preston, M.; Tegnér, P. E.; Wölbing, D.; Bäck, T.; Cederwall, B.; Kumar, Ajay; Godre, S.; Calvo, D.; Coli, S.; Remigis, P. De; Filippi, A.; Giraudo, G.; Lusso, S.; Mazza, G.; Mignone, M.; Rivetti, A.; Wheadon, R.; Balestra, F.; Iazzi, F.; Introzzi, R.; Lavagno, Andrea; Olave, J.; Amoroso, A.; Bussa, M. P.; Busso, L.; Mori, F. De; Destefanis, M.; Fava, L.; Ferrero, L.; Greco, M.; Hu, J. F.; Lavezzi, L.; Maggiora, M.; Maniscalco, G.; Marcello, S.; Sosio, S.; Spataro, S.; Birsa, R.; Bradamante, F.; Bressan, A.; Martin, A.; Calén, H.; Andersson, W. Ikegami; Johansson, T.; Kupść, A.; Marciniewski, P.; Papenbrock, M.; Pettersson, J.; Schönning, K.; Wolke, M.; Gålnander, Björn; Díaz, J.; Chackara, V. Pothodi; Chłopik, A.; Kȩsik, G.; Melnychuk, D.; Słowiński, B.; Trzciński, A.; Wojciechowski, M.; Wronka, S.; Zwiȩgliński, B.; Bühler, P.; Márton, J.; Steinschaden, D.; Suzuki, K.; Widmann, E.; Zmeskal, J.

doi:10.1140/epja/i2016-16325-5

Cited by 34 publications

(4 citation statements)

References 69 publications

(68 reference statements)

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“…The BESIII Collaboration observed (1530) in a baryon-antibaryon pair from charmonium decay [9]. The upcoming experimental facility PANDA at FAIR-GSI has high expectations to establish the whole spectrum of hyperons through proton-antiproton collisions [10][11][12][13]. A dedicated study has been undertaken for mass, width, and decay modes by a member of the PANDA group [14][15][16].…”

Section: Introductionmentioning

confidence: 99%

Spectroscopic investigation of light strange S = −1 Λ and Σ and S = −2 Ξ baryons

Menapara

Kumar

2021

Chinese Phys. C

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The present study is dedicated to light-strange Λ with strangeness S=-1, isospin I=0; Σ with S=-1, I=1 and Ξ baryon with S=-2 and I = 1 2 . In this article, hypercentral Constituent Quark Model with linear confining potential has been employed along with first order correction term to obtain the resonance masses for nearly upto 4 GeV. The calculated states include 1S-5S, 1P-4P, 1D-3D, 1F-2F and 1G (in few case) along with all the possible spin-parity assignments. Regge Trajectories have been explored for the linearly of the calculated masses for (n, M 2 ) and (J, M 2 ) respectively. Magnetic moments have been intensively studied for ground state spin 1 2 and 3 2 , in addition to the configuration mixing for first negative parity state for Ξ. Lastly, transition magnetic moment and radiative decay width have been presented.

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Section: Introductionmentioning

confidence: 99%

Spectroscopic investigation of light strange S = −1 Λ and Σ and S = −2 Ξ baryons

Menapara

Kumar

2021

Chinese Phys. C

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“…The second channel will be the first access to proton TL EM FFs using leptons other than electrons, which will also allow for tests of lepton universality. Feasibility studies exist for both channels: for the electron channel [39], the expected relative uncertainties range between 1% and 5% for the FF ratio (|G E /G M |) and 1% and 4% for |G E | in the already explored q 2 range up to 3 GeV/c. The expected uncertainty for both R and |G E | grows to more than 50% at 3.73 GeV/c.…”

Section: Future Experimental Prospectsmentioning

confidence: 99%

Proton Electromagnetic Form Factors in the Time-like Region through the Scan Technique

et al. 2022

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For over 100 y, scientists have investigated the properties of the proton, which is one of the most abundant components of visible matter in the universe. Nevertheless, researchers do not fully understand many details about its internal structure and dynamics. Time-like electromagnetic form factors are some of the observable quantities that can help us achieve a deeper understanding. In this review article, we present an overview of the current experimental status in this field, consisting of measurements of the time-like reactions e+e−→pp¯ and pp¯→e+e− and future measurements of pp¯→μ+μ−. The focus is put on recent high-precision results of the reaction e+e−→pp¯ that have been obtained after analyzing 688.5 pb−1 of data taken at the BESIII experiment. They are compared to and put into perspective with results from previous measurements in this channel. We discuss the channels pp¯→e+e− and pp¯→μ+μ− in terms of the few existing, as well as future measurements, which the PANDA experiment will perform. Finally, we review several new theoretical models and phenomenological approaches inspired by the BESIII high-precision results and then discuss their implications for a deeper understanding of the proton’s structure and inner dynamics.

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“…The modulus of the time-like proton FFs will be measured at PANDA in the annihilation processes pp → e + e − and pp → µ + µ − . Feasibility studies for the measurement of these two processes at PANDA have been performed based on Monte Carlo simulations within the PANDARoot framework at different q 2 values between 5 (GeV/c) 2 and 14 (GeV/c) 2 [2,5,6]. The difficulty of these measurements is related to the hadronic background, mainly from the annihilation process pp → π + π − .…”

Section: Measurements Of the Proton Electromagnetic Form Factors At P...mentioning

confidence: 99%

Study of the nucleon structure with the PANDA experiment at FAIR

Dbeyssi¹

2022

Proceedings of Particles and Nuclei International Conference 2021 — PoS(PANIC2021)

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The PANDA experiment is a core project of the future Facility for Antiproton and Ion Research (FAIR) at GSI in Darmstadt. It will measure annihilation reactions induced by a high intensity antiproton beam of momentum in the range between 1.5 GeV/c and 15 GeV/c. An important part of the PANDA physics program will be dedicated to the investigation of the nucleon structure using electromagnetic processes. Measurements of the proton electromagnetic form factors in the time-like region, nucleon-to-meson transition distribution amplitudes, generalised distribution amplitudes, and transverse momentum dependent parton distribution functions, are foreseen at PANDA. In the framework of the PANDARoot software, which encompasses PANDA detector simulation and event reconstruction, feasibility studies for the measurement of various electromagnetic processes have been performed. It has been shown that unique studies of the nucleon structure can be experimentally performed at PANDA. In this report, the physics program of PANDA related to the study of the electromagnetic form factors and the transition distribution amplitudes is described with the results of the Monte Carlo feasibility studies.

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Feasibility studies of time-like proton electromagnetic form factors at $\overline{\rm P}$ P ¯ ANDA at FAIR

Cited by 34 publications

References 69 publications

Spectroscopic investigation of light strange S = −1 Λ and Σ and S = −2 Ξ baryons

Spectroscopic investigation of light strange S = −1 Λ and Σ and S = −2 Ξ baryons

Proton Electromagnetic Form Factors in the Time-like Region through the Scan Technique

Study of the nucleon structure with the PANDA experiment at FAIR

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