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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

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 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

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

One of the goals of hypernuclear physics is to study the properties of baryon-baryon interaction including the strangeness contribution. Double hypernuclei can provide information about the $\Lambda\Lambda$ interaction in addition to the…

High Energy Physics - Experiment · Physics 2008-10-16 Katarzyna Szymanska

The technical design of the PANDA experiment at the future FAIR facility next to GSI is progressing. At the proposed anti-proton storage ring the spectroscopy of double Lambda hypernuclei is one of the four main topics which will be…

Instrumentation and Detectors · Physics 2011-06-22 P. Achenbach , J. Pochodzalla , A. Sanchez Lorente , S. Sánchez Majos

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 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

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

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

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

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

Hypernuclear research will be one of the main topics addressed by the PANDA experiment at the planned Facility for Anti-proton and Ion Research FAIR at Darmstadt, Germany. A copious production of Xi-hyperons at a dedicated internal target…

Nuclear Experiment · Physics 2012-06-15 P. Achenbach , S. Bleser , J. Pochodzalla , A. Sanchez Lorente , M. Steinen

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 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

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

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 $\overline{\mbox{P}}$ANDA experiment together with the high quality antiproton beam at HESR will be a powerful tool to address fundamental questions of hadron physics in the charm and multi-strange hadron sector. In connection with the…

High Energy Physics - Experiment · Physics 2015-12-11 PANDA Collaboration , Nora Brambilla , Ulf-G. Meißner

A major ingredient of the planned new accelerator complex FAIR, to be constructed at the GSI, Darmstadt, Germany, is the availability of antiproton beams with high quality and intensity. Among the experiments which will make use of this…

Nuclear Experiment · Physics 2009-11-11 O. N. Hartmann
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