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The Anti-Proton ANnihilation at DArmstadt (PANDA) experiment proposed at the Facility for Antiproton and Ion Research (FAIR) in Darmstadt (Germany) will perform a high precision spectroscopy of charmonium and exotic hadrons, such as…

Computational Physics · Physics 2019-08-13 Aleksandra Biegun

In the PANDA experiment at the FAIR facility at GSI two DIRC (Detection of Internally Reflected Cherenkov light) detectors will be used for $\pi$/K separation up to 4 GeV/c. Due to their location in a high magnetic field and other stringent…

The barrel time-of-flight detector for the PANDA experiment at FAIR is foreseen as a Scintillator Tile (SciTil) Hodoscope based on several thousand small plastic scintillator tiles read-out with directly attached Silicon Photomultipliers…

Instrumentation and Detectors · Physics 2019-08-14 L. Gruber , S. E. Brunner , J. Marton , H. Orth , K. Suzuki

The PANDA experiment at the FAIR facility at GSI will study hadron physics using a high intensity antiproton beam of up to 15 GeV/c momentum to perform high precision spectroscopy. Two DIRC detectors with their image planes residing in an…

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 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 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

To study fundamental questions of hadron and nuclear physics in interactions of antiprotons with nucleons and nuclei, the universal PANDA detector will be built. Gluonic excitations, the physics of strange and charm quarks and nucleon…

High Energy Physics - Experiment · Physics 2019-08-17 PANDA Collaboration , W. Erni , I. Keshelashvili , B. Krusche , M. Steinacher , Y. Heng , Z. Liu , H. Liu , X. Shen , O. Wang , H. Xu , J. Becker , F. Feldbauer , F. -H. Heinsius , T. Held , H. Koch , B. Kopf , M. Pelizaeus , T. Schroeder , M. Steinke , U. Wiedner , J. Zhong , A. Bianconi , M. Bragadireanu , D. Pantea , A. Tudorache , V. Tudorache , M. De Napoli , F. Giacoppo , G. Raciti , E. Rapisarda , C. Sfienti , E. Bialkowski , A. Budzanowski , B. Czech , M. Kistryn , S. Kliczewski , A. Kozela , P. Kulessa , K. Pysz , W. Schaefer , R. Siudak , A. Szczurek , W. Czy. zycki , M. Domagala , M. Hawryluk , E. Lisowski , F. Lisowski , L. Wojnar , D. Gil , P. Hawranek , B. Kamys , St. Kistryn , K. Korcyl , W. Krzemien , A. Magiera , P. Moskal , Z. Rudy , P. Salabura , J. Smyrski , A. Wronska , M. Al-Turany , I. Augustin , H. Deppe , H. Flemming , J. Gerl , K. Goetzen , R. Hohler , D. Lehmann , B. Lewandowski , J. Luehning , F. Maas , D. Mishra , H. Orth , K. Peters , T. Saito , G. Schepers , C. J. Schmidt , L. Schmitt , C. Schwarz , B. Voss , P. Wieczorek , A. Wilms , K. -T. Brinkmann , H. Freiesleben , R. Jaekel , R. Kliemt , T. Wuerschig , H. -G. Zaunick , V. M. Abazov , G. Alexeev , A. Arefiev , V. I. Astakhov , M. Yu. Barabanov , B. V. Batyunya , Yu. I. Davydov , V. Kh. Dodokhov , A. A. Efremov , A. G. Fedunov , A. A. Feshchenko , A. S. Galoyan , S. Grigoryan , A. Karmokov , E. K. Koshurnikov , V. Ch. Kudaev , V. I. Lobanov , Yu. Yu. Lobanov , A. F. Makarov , L. V. Malinina , V. L. Malyshev , G. A. Mustafaev , A. Olshevski , M. A. Pasyuk , E. A. Perevalova , A. A. Piskun , T. A. Pocheptsov , G. Pontecorvo , V. K. Rodionov , Yu. N. Rogov , R. A. Salmin , A. G. Samartsev , M. G. Sapozhnikov , A. Shabratova , G. S. Shabratova , A. N. Skachkova , N. B. Skachkov , E. A. Strokovsky , M. K. Suleimanov , R. Sh. Teshev , V. V. Tokmenin , V. V. Uzhinsky , A. S. Vodopianov , S. A. Zaporozhets , N. I. Zhuravlev , A. G. Zorin , D. Branford , K. Foehl , D. Glazier , D. Watts , P. Woods , W. Eyrich , A. Lehmann , A. Teufel , S. Dobbs , Z. Metreveli , K. Seth , B. Tann , A. Tomaradze , D. Bettoni , V. Carassiti , A. Cecchi , P. Dalpiaz , E. Fioravanti , I. Garzia , M. Negrini , M. Savri`e , G. Stancari , B. Dulach , P. Gianotti , C. Guaraldo , V. Lucherini , E. Pace , A. Bersani , M. Macri , M. Marinelli , R. F. Parodi , I. Brodski , W. Doering , P. Drexler , M. Dueren , Z. Gagyi-Palffy , A. Hayrapetyan , M. Kotulla , W. Kuehn , S. Lange , M. Liu , V. Metag , M. Nanova , R. Novotny , C. Salz , J. Schneider , P. Schoenmeier , R. Schubert , S. Spataro , H. Stenzel , C. Strackbein , M. Thiel , U. Thoering , S. Yang , T. Clarkson , E. Cowie , E. Downie , G. Hill , M. Hoek , D. Ireland , R. Kaiser , T. Keri , I. Lehmann , K. Livingston , S. Lumsden , D. MacGregor , B. McKinnon , M. Murray , D. Protopopescu , G. Rosner , B. Seitz , G. Yang , M. Babai , A. K. Biegun , A. Bubak , E. Guliyev , V. S. Jothi , M. Kavatsyuk , H. Loehner , J. Messchendorp , H. Smit , J. C. van der Weele , F. Garcia , D. -O. Riska , M. Buescher , R. Dosdall , R. Dzhygadlo , A. Gillitzer , D. Grunwald , V. Jha , G. Kemmerling , H. Kleines , A. Lehrach , R. Maier , M. Mertens , H. Ohm , D. Prasuhn , T. Randriamalala , J. Ritman , M. Roeder , T. Stockmanns , P. Wintz , P. Wuestner , J. Kisiel , S. Li , Z. Li , Z. Sun , H. Xu , S. Fissum , K. Hansen , L. Isaksson , M. Lundin , B. Schroeder , P. Achenbach , M. C. Mora Espi , J. Pochodzalla , S. Sanchez , A. Sanchez-Lorente , V. I. Dormenev , A. A. Fedorov , M. V. Korzhik , O. V. Missevitch , V. Balanutsa , V. Chernetsky , A. Demekhin , A. Dolgolenko , P. Fedorets , A. Gerasimov , V. Goryachev , A. Boukharov , O. Malyshev , I. Marishev , A. Semenov , C. Hoeppner , B. Ketzer , I. Konorov , A. Mann , S. Neubert , S. Paul , Q. Weitzel , A. Khoukaz , T. Rausmann , A. Taeschner , J. Wessels , R. Varma , E. Baldin , K. Kotov , S. Peleganchuk , Yu. Tikhonov , J. Boucher , T. Hennino , R. Kunne , S. Ong , J. Pouthas , B. Ramstein , P. Rosier , M. Sudol , J. Van de Wiele , T. Zerguerras , K. Dmowski , R. Korzeniewski , D. Przemyslaw , B. Slowinski , G. Boca , A. Braghieri , S. Costanza , A. Fontana , P. Genova , L. Lavezzi , P. Montagna , A. Rotondi , N. I. Belikov , A. M. Davidenko , A. A. Derevschikov , Y. M. Goncharenko , V. N. Grishin , V. A. Kachanov , D. A. Konstantinov , V. A. Kormilitsin , V. I. Kravtsov , Y. A. Matulenko , Y. M. Melnik , A. P. Meschanin , N. G. Minaev , V. V. Mochalov , D. A. Morozov , L. V. Nogach , S. B. Nurushev , A. V. Ryazantsev , P. A. Semenov , L. F. Soloviev , A. V. Uzunian , A. N. Vasiliev , A. E. Yakutin , T. Baeck , B. Cederwall , C. Bargholtz , L. Geren , P. E. Tegner , S. Belostotski , G. Gavrilov , A. Itzotov , A. Kisselev , P. Kravchenko , S. Manaenkov , O. Miklukho , Y. Naryshkin , D. Veretennikov , V. Vikhrov , A. Zhadanov , L. Fava , D. Panzieri , D. Alberto , A. Amoroso , E. Botta , T. Bressani , S. Bufalino , M. P. Bussa , L. Busso , F. De Mori , M. Destefanis , L. Ferrero , A. Grasso , M. Greco , T. Kugathasan , M. Maggiora , S. Marcello , G. Serbanut , S. Sosio , R. Bertini , D. Calvo , S. Coli , P. De Remigis , A. Feliciello , A. Filippi , G. Giraudo , G. Mazza , A. Rivetti , K. Szymanska , F. Tosello , R. Wheadon , O. Morra , M. Agnello , F. Iazzi , K. Szymanska , R. Birsa , F. Bradamante , A. Bressan , A. Martin , H. Clement , C. Ekstroem , H. Calen , S. Grape , B. Hoeistad , T. Johansson , A. Kupsc , P. Marciniewski , E. Thome , J. Zlomanczuk , J. Diaz , A. Ortiz , S. Borsuk , A. Chlopik , Z. Guzik , J. Kopec , T. Kozlowski , D. Melnychuk , M. Plominski , J. Szewinski , K. Traczyk , B. Zwieglinski , P. Buehler , A. Gruber , P. Kienle , J. Marton , E. Widmann , J. Zmeskal , M. F. M. Lutz , B. Pire , O. Scholten , R. Timmermans

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 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 will be built at the FAIR facility at Darmstadt (Germany) to perform accurate tests of the strong interaction through bar pp and bar pA annihilation's studies. To track charged particles, two systems consisting of a set…

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

The DIRC, a new type of Cherenkov imaging device, has been selected as the primary particle identification system for the BABAR detector at the asymmetric B-factory, PEP-II. It is based on total internal reflection and uses long,…

High Energy Physics - Experiment · Physics 2015-06-25 Jochen Schwiening

The DIRC is a new type of Cherenkov detector that is successfully operating as the hadronic particle identification system for the BABAR experiment at SLAC. The fused silica bars that serve as the DIRC's Cherenkov radiators must transmit…

High Energy Physics - Experiment · Physics 2015-06-25 M. Convery , B. Ratcliff , X. Sarazin , J. Schwiening , J. Va'vra

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

We present the final results from a novel Cherenkov imaging detector called the Focusing DIRC (FDIRC). This detector was designed as a full-scale prototype of the particle identification system for the SuperB experiment [1], and comprises…

Instrumentation and Detectors · Physics 2015-12-09 B. Dey , M. Borsato , N. Arnaud , D. W. G. S. Leith , K. Nishimura , D. A. Roberts , B. N. Ratcliff , G. Varner , J. Va'vra

The DIRC, a novel type of Cherenkov ring imaging device, is the primary hadronic particle identification system for the BaBar detector at the asymmetric B-factory Pep-II at SLAC. It is based on total internal reflection and uses long,…

High Energy Physics - Experiment · Physics 2007-05-23 T. Hadig

The study of baryon excitation spectra provides insight into the inner structure of baryons. So far, most of the world-wide efforts have been directed towards $N^*$ and $\Delta$ spectroscopy. Nevertheless, the study of the double and triple…

High Energy Physics - Experiment · Physics 2021-04-28 PANDA Collaboration

The Electron-ion collider in China (EicC) is a proposed future electron-ion collider designed to achieve a high luminosity, with a center-of-mass energy ranging from 15 to 20 GeV. Excellent particle identification (PID) with extensive…

Instrumentation and Detectors · Physics 2026-05-25 Xin Li , Yuxiang Zhao , Yutie Liang , Xu Sun

The DIRC is a new type of Cherenkov imaging device that will be used for the first time in the BABAR detector at the asymmetric B-factory, PEP-II. It is based on total internal reflection and uses long, rectangular bars made from synthetic…

High Energy Physics - Experiment · Physics 2015-06-25 DIRC Collaboration