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Related papers: Strong interaction studies with PANDA

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Quantum Chromodynamics (QCD) is the fundamental theory of strong interactions. It describes the behavior of quarks and gluons which are the smallest known constituents of nuclear matter. The difficulties in solving the theory at low…

High Energy Physics - Phenomenology · Physics 2009-12-22 Theodor Brasoveanu , Dmitri Kharzeev , Mauricio Martinez

Studies of the spectrum of hadrons and their structure in experiments with electromagnetic probes offer unique insight into many facets of the strong interaction in the regime of large quark-gluon running coupling, {\it i.e.} the regime of…

Nuclear Experiment · Physics 2020-08-26 D. S. Carman , K. Joo , V. I. Mokeev

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

We highlight the progress, current status, and open challenges of QCD-driven physics, in theory and in experiment. We discuss how the strong interaction is intimately connected to a broad sweep of physical problems, in settings ranging from…

QCD, the theory of the strong interactions, involves quarks interacting with non-Abelian gluon fields. This theory has many features that are difficult to impossible to see in conventional diagrammatic perturbation theory. This includes…

High Energy Physics - Phenomenology · Physics 2021-09-01 Michael Creutz

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

This chapter provides a pedagogical introduction to theoretical studies of hadrons based on the fundamental theory of strong interactions - Quantum ChromoDynamics. A perturbative expansion in the strong coupling is not applicable at…

High Energy Physics - Lattice · Physics 2025-05-16 Sasa Prelovsek

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

Quantum Chromo Dynamics (QCD), the theory of strong interactions, predicts a transition of the usual matter to a new phase of matter, called Quark-Gluon Plasma (QGP), at sufficiently high temperatures. The non-perturbative technique of…

High Energy Physics - Phenomenology · Physics 2015-05-13 Rajeev S. Bhalerao , Rajiv V. Gavai

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…

This writeup summarizes the main experimental studies of the strong interaction, theoretically described by quantum chromodynamics (QCD), that were presented during the ICHEP-2020 conference. The latest results, measured mostly in p-p…

High Energy Physics - Experiment · Physics 2020-12-15 David d'Enterria

Unlike some models whose relevance to Nature is still a big question mark, Quantum Chromodynamics will stay with us forever. Quantum Chromodynamics (QCD), born in 1973, is a very rich theory supposed to describe the widest range of strong…

High Energy Physics - Theory · Physics 2009-11-11 M. Shifman

This review deals with the structure of hadrons, strongly interacting many-body systems consisting of quarks and gluons. These systems have a size of about 1 fm, which shows up in scattering experiments at low momentum transfers $Q$ in the…

High Energy Physics - Phenomenology · Physics 2009-09-29 Dieter Drechsel , Thomas Walcher

Since QCD is believed to be the underlying theory of the strong interaction, it is appropriate to study techniques that take into account more features of its rich and complex structure. We begin by discussing aspects of physics that are…

Nuclear Theory · Physics 2007-05-23 Richard F. Lebed

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

Matter described by Quantum Chromodynamics (QCD), the theory of strong interactions, may undergo phase transitions when its temperature and the chemical potentials are varied. QCD at finite temperature is studied in the laboratory by…

High Energy Physics - Phenomenology · Physics 2011-06-24 Sourendu Gupta , Xiaofeng Luo , Bedangadas Mohanty , Hans Georg Ritter , Nu Xu

Despite the progress made in understanding the NN interactions at long distances based on effective field theories, the understanding of the dynamics of short range NN interactions remains as elusive as ever. One of the most fascinating…

Nuclear Theory · Physics 2014-03-05 Misak M Sargsian

Quantum Chromodynamics (QCD), the gauge field theory of the Strong Interaction, has specific features, asymptotic freedom and confinement, which determine the behaviour of quarks and gluons in particle reactions at high and at low energy…

High Energy Physics - Experiment · Physics 2008-11-26 Siegfried Bethke

Exploration of the small $x$ kinematic region by the HERA experiments led to a revival of some models which existed before the advent of Quantum Chromo Dynamics (QCD) as the theory of the strong interactions. Predictions of these models for…

High Energy Physics - Phenomenology · Physics 2009-10-31 W. L. van Neerven

According to the present understanding, the observed diversity of the strong interaction phenomena is described by Quantum Chromodynamics, a gauge field theory with only very few parameters. One of the fundamental questions in this context…

High Energy Physics - Phenomenology · Physics 2009-11-07 Martin Lüscher