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Related papers: Studies of Hadron Structure and Interactions with …

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The non-perturbative nature of the strong interaction leads to spectacular phenomena, such as the formation of hadronic matter, color confinement, and the generation of the mass of visible matter. To get deeper insight into the underlying…

Nuclear Experiment · Physics 2019-08-13 Johan Messchendorp

The PANDA experiment at the new FAIR facility will be the major hadron physics experiment at the end of this decade. It has an ambitious far-reaching physics program that spans the most fascinating topics that are emerging in contemporary…

High Energy Physics - Experiment · Physics 2011-06-08 Ulrich Wiedner

Physics with antiprotons in the charmonium mass region will play a major role at the future PANDA experiment at the FAIR facility in Darmstadt. At PANDA, an antiproton beam with momenta up to 15 GeV/c circulating in the high-energy storage…

Instrumentation and Detectors · Physics 2013-12-18 Kai-Thomas Brinkmann

The $\bar PANDA$ experiment at FAIR (Facility for Antiproton and Ion Research) in Darmstadt (Germany) is designed for $\bar p p$ annihilation studies and it will investigate fundamental questions of hadron and nuclear physics in…

High Energy Physics - Experiment · Physics 2014-10-28 Elisabetta Prencipe

FAIR a new International Facility for Antiproton and Ion Reaserach, is under construction at Darmstadt, in Germany. This will provide scientists in the world with outstanding beams and experimental conditions for studying matter at the…

High Energy Physics - Experiment · Physics 2019-08-13 Elisa Fioravanti

The physics program of the future FAIR facility covers a wide range of topics that address central issues of strong interactions and QCD. The antiproton beam of unprecedented quality in the momentum range from 1 GeV/c to 15 GeV/c will allow…

High Energy Physics - Experiment · Physics 2011-06-15 Diego Bettoni

Exciting new scientific opportunities are presented for the PANDA detector at the High Energy Storage Ring in the redefined $\bar{\text{p}} \text{p}(A)$ collider mode, HESR-C, at the Facility for Antiproton and Ion Research (FAIR) in…

The PANDA detector is under design to be installed at the HESR storage ring for antiproton of the future FAIR facility in Darmstadt, Germany. Fundamental questions of hadron and nuclear physics interactions of antiprotons with nucleons and…

Instrumentation and Detectors · Physics 2008-10-16 S. Marcello

The Facility for Antiproton and Ion Research (FAIR) in Darmstadt, Germany, provides unique possibilities for a new generation of hadron-, nuclear- and atomic physics experiments. The future antiProton ANnihilations at DArmstadt (PANDA or…

High Energy Physics - Experiment · Physics 2021-06-10 G. Barucca , F. Davì , G. Lancioni , P. Mengucci , L. Montalto , P. P. Natali , N. Paone , D. Rinaldi , L. Scalise , B. Krusche , M. Steinacher , Z. Liu , C. Liu , B. Liu , X. Shen , S. Sun , G. Zhao , J. Zhao , M. Albrecht , W. Alkakhi , S. Bökelmann , S. Coen , F. Feldbauer , M. Fink , J. Frech , V. Freudenreich , M. Fritsch , J. Grochowski , R. Hagdorn , F. H. Heinsius , T. Held , T. Holtmann , I. Keshk , H. Koch , B. Kopf , M. Kümmel , M. Küßner , J. Li , L. Linzen , S. Maldaner , J. Oppotsch , S. Pankonin , M. Pelizäus , S. Pflüger , J. Reher , G. Reicherz , C. Schnier , M. Steinke , T. Triffterer , C. Wenzel , U. Wiedner , H. Denizli , N. Er , U. Keskin , S. Yerlikaya , A. Yilmaz , R. Beck , V. Chauhan , C. Hammann , J. Hartmann , B. Ketzer , J. Müllers , B. Salisbury , C. Schmidt , U. Thoma , M. Urban , A. Bianconi , M. Bragadireanu , D. Pantea , S. Rimjaem , M. Domagala , G. Filo , E. Lisowski , F. Lisowski , M. Michałek , P. Poznański , J. Płażek , K. Korcyl , P. Lebiedowicz , K. Pysz , W. Schäfer , A. Szczurek , M. Firlej , T. Fiutowski , M. Idzik , J. Moron , K. Swientek , P. Terlecki , G. Korcyl , R. Lalik , A. Malige , P. Moskal , K. Nowakowski , W. Przygoda , N. Rathod , P. Salabura , J. Smyrski , I. Augustin , R. Böhm , I. Lehmann , L. Schmitt , V. Varentsov , M. Al-Turany , A. Belias , H. Deppe , R. Dzhygadlo , H. Flemming , A. Gerhardt , K. Götzen , A. Heinz , P. Jiang , R. Karabowicz , S. Koch , U. Kurilla , D. Lehmann , J. Lühning , U. Lynen , H. Orth , K. Peters , J. Ritman , G. Schepers , C. J. Schmidt , C. Schwarz , J. Schwiening , A. Täschner , M. Traxler , B. Voss , P. Wieczorek , V. Abazov , G. Alexeev , M. Yu. Barabanov , V. Kh. Dodokhov , A. Efremov , A. Fechtchenko , A. Galoyan , G. Golovanov , E. K. Koshurnikov , Y. Yu. Lobanov , A. G. Olshevskiy , A. A. Piskun , A. Samartsev , S. Shimanski , N. B. Skachkov , A. N. Skachkova , E. A. Strokovsky , V. Tokmenin , V. Uzhinsky , A. Verkheev , A. Vodopianov , N. I. Zhuravlev , D. Watts , M. Böhm , W. Eyrich , A. Lehmann , D. Miehling , M. Pfaffinger , K. Seth , T. Xiao , A. Ali , A. Hamdi , M. Himmelreich , M. Krebs , S. Nakhoul , F. Nerling , P. Gianotti , V. Lucherini , G. Bracco , S. Bodenschatz , K. T. Brinkmann , L. Brück , S. Diehl , V. Dormenev , M. Düren , T. Erlen , C. Hahn , A. Hayrapetyan , J. Hofmann , S. Kegel , F. Khalid , I. Köseoglu , A. Kripko , W. Kühn , V. Metag , M. Moritz , M. Nanova , R. Novotny , P. Orsich , J. Pereira-de-Lira , M. Sachs , M. Schmidt , R. Schubert , M. Strickert , T. Wasem , H. G. Zaunick , E. Tomasi-Gustafsson , D. Glazier , D. Ireland , B. Seitz , R. Kappert , M. Kavatsyuk , H. Loehner , J. Messchendorp , V. Rodin , K. Kalita , G. Huang , D. Liu , H. Peng , H. Qi , Y. Sun , X. Zhou , M. Kunze , K. Azizi , A. T. Olgun , Z. Tavukoglu , A. Derichs , R. Dosdall , W. Esmail , A. Gillitzer , F. Goldenbaum , D. Grunwald , L. Jokhovets , J. Kannika , P. Kulessa , S. Orfanitski , G. Perez-Andrade , D. Prasuhn , E. Prencipe , J. Pütz , E. Rosenthal , S. Schadmand , R. Schmitz , A. Scholl , T. Sefzick , V. Serdyuk , T. Stockmanns , D. Veretennikov , P. Wintz , P. Wüstner , H. Xu , Y. Zhou , X. Cao , Q. Hu , Y. Liang , V. Rigato , L. Isaksson , P. Achenbach , O. Corell , A. Denig , M. Distler , M. Hoek , W. Lauth , H. H. Leithoff , H. Merkel , U. Müller , J. Petersen , J. Pochodzalla , S. Schlimme , C. Sfienti , M. Thiel , S. Bleser , M. Bölting , L. Capozza , A. Dbeyssi , A. Ehret , R. Klasen , R. Kliemt , F. Maas , C. Motzko , O. Noll , D. Rodríguez Piñeiro , F. Schupp , M. Steinen , S. Wolff , I. Zimmermann , D. Kazlou , M. Korzhik , O. Missevitch , P. Balanutsa , V. Chernetsky , A. Demekhin , A. Dolgolenko , P. Fedorets , A. Gerasimov , A. Golubev , A. Kantsyrev , D. Y. Kirin , N. Kristi , E. Ladygina , E. Luschevskaya , V. A. Matveev , V. Panjushkin , A. V. Stavinskiy , A. Balashoff , A. Boukharov , M. Bukharova , O. Malyshev , E. Vishnevsky , D. Bonaventura , P. Brand , B. Hetz , N. Hüsken , J. Kellers , A. Khoukaz , D. Klostermann , C. Mannweiler , S. Vestrick , D. Bumrungkoh , C. Herold , K. Khosonthongkee , C. Kobdaj , A. Limphirat , K. Manasatitpong , T. Nasawad , S. Pongampai , T. Simantathammakul , P. Srisawad , N. Wongprachanukul , Y. Yan , C. Yu , X. Zhang , W. Zhu , E. Antokhin , A. Yu. Barnyakov , K. Beloborodov , V. E. Blinov , I. A. Kuyanov , S. Pivovarov , E. Pyata , Y. Tikhonov , A. E. Blinov , S. Kononov , E. A. Kravchenko , M. Lattery , G. Boca , D. Duda , M. Finger , M. Finger, , A. Kveton , I. Prochazka , M. Slunecka , M. Volf , V. Jary , O. Korchak , M. Marcisovsky , G. Neue , J. Novy , L. Tomasek , M. Tomasek , M. Virius , V. Vrba , V. Abramov , S. Bukreeva , S. Chernichenko , A. Derevschikov , V. Ferapontov , Y. Goncharenko , A. Levin , E. Maslova , Y. Melnik , A. Meschanin , N. Minaev , V. Mochalov , V. Moiseev , D. Morozov , L. Nogach , S. Poslavskiy , A. Ryazantsev , S. Ryzhikov , P. Semenov , I. Shein , A. Uzunian , A. Vasiliev , A. Yakutin , S. Belostotski , G. Fedotov , A. Izotov , S. Manaenkov , O. Miklukho , B. Cederwall , M. Preston , P. E. Tegner , D. Wölbing , K. Gandhi , A. K. Rai , S. Godre , V. Crede , S. Dobbs , P. Eugenio , M. P. Bussa , S. Spataro , D. Calvo , P. De Remigis , A. Filippi , G. Mazza , R. Wheadon , F. Iazzi , A. Lavagno , A. Akram , H. Calen , W. Ikegami Andersson , T. Johansson , A. Kupsc , P. Marciniewski , M. Papenbrock , J. Regina , J. Rieger , K. Schönning , M. Wolke , A. Chlopik , G. Kesik , D. Melnychuk , J. Tarasiuk , M. Wojciechowski , S. Wronka , B. Zwieglinski , C. Amsler , P. Bühler , J. Marton , S. Zimmermann , C. S. Fischer , J. Haidenbauer , C. Hanhart , M. F. M. Lutz , Sinéad M. Ryan

The theory of Quantum Chromo Dynamics (QCD) reproduces the strong interaction at distances much shorter than the size of the nucleon. At larger distance scales, the generation of hadron masses and confinement cannot yet be derived from…

Nuclear Experiment · Physics 2011-06-30 J. G. Messchendorp

Exciting new scientific opportunities are presented for the PANDA detector at the High Energy Storage Ring in the redefined $\overline{\text{p}} \text{p}(A)$ collider mode, HESR-C, at the Facility for Antiproton and Ion Research (FAIR) in…

The Facility for Antiproton and Ion Research (FAIR) is an international accelerator facility which will use antiprotons and ions to perform research in the fields of nuclear, hadron and particle physics, atomic and anti-matter physics, high…

High Energy Physics - Experiment · Physics 2014-11-06 Elisabetta Prencipe

The standard model and Quantum Chromodynamics (QCD) have undergone rigorous tests at distances much shorter than the size of a nucleon. Up to now, the predicted phenomena are reproduced rather well. However, at distances comparable to the…

High Energy Physics - Experiment · Physics 2019-08-13 Inti Lehmann

PANDA, the detector to study AntiProton ANnihilations at DArmstadt, will be installed at the future international Facility for Anti-proton and Ion Research (FAIR) in Darmstadt, Germany. The PANDA physics program is oriented towards the…

Computational Physics · Physics 2019-08-13 A. Biegun

One component of the future international Facility for Antiproton and Ion Research - FAIR is directed towards studies of hadronic matter at the sub-nuclear level with beams of antiprotons. These studies focus on two key aspects: confinement…

High Energy Physics - Experiment · Physics 2008-11-26 James Ritman

The antiproton experiment PANDA at FAIR is designed to bring hadron physics to a new level in terms of scope, precision and accuracy. In this work, its unique capability for studies of hyperons is outlined. We discuss ground-state hyperons…

High Energy Physics - Experiment · Physics 2021-05-27 The PANDA Collaboration

The PANDA detector at FAIR aims to conduct an antiproton-proton experiment with a very high rate capability. It is expected to feature high mass resolution, more than 20 times better than achieved at B-factories. PANDA is in a unique…

High Energy Physics - Experiment · Physics 2015-10-13 Elisabetta Prencipe

The theory of Quantum Chromo Dynamics (QCD) reproduces the strong interaction at distances much shorter than the size of the nucleon. At larger distance scales, the generation of hadron masses and confinement cannot yet be derived from…

High Energy Physics - Experiment · Physics 2019-08-13 J. G. Messchendorp

With the PANDA detector at the HESR at FAIR it will be possible to study the production and absorption of charmed hadrons in nuclear targets. Of special interest in this context is the determination of the JPsi-nucleon dissociation cross…

Nuclear Experiment · Physics 2011-09-20 Paul Bühler

The physics of strong interactions is undoubtedly one of the most challenging areas of modern science. The PANDA experiment will be devoted to charmonium spectroscopy, gluonic excitations (hybrids, glueballs), open and hidden charm in…

Instrumentation and Detectors · Physics 2007-05-23 Kai-Thomas Brinkmann , Paola Gianotti , Inti Lehmann
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