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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 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. BABAR began taking data with colliding beams mode in late…

High Energy Physics - Experiment · Physics 2007-05-23 Jochen Schwiening , representing the BABAR-DIRC Collaboration

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 DIRAC spectrometer has been commissioned at CERN with the aim of detecting $\pi^+ \pi^-$ atoms produced by a 24 GeV/$c$ high intensity proton beam in thin foil targets. A challenging apparatus is required to cope with the high…

High Energy Physics - Experiment · Physics 2012-08-27 DIRAC Collaboration

The DIRC is a Cherenkov imaging detector based on total internal reflection for the BaBar detector at PEP-II. The principles of the DIRC ring imaging Cherenkov technique are explained and its choice for the BaBar detector particle…

High Energy Physics - Experiment · Physics 2009-10-30 J. Schwiening

The Electron-Ion Collider (EIC) will be the next frontier project of nuclear physics in the United States. It is planned to be built in the Brookhaven National Laboratory (BNL) in close collaboration with Jefferson Lab. One of the key…

Instrumentation and Detectors · Physics 2022-02-15 Greg Kalicy

The PANDA detection system at FAIR, Germany, is designed to study antiproton-proton annihilations, in order to investigate among others the realm of charm-meson states and glueballs, which has still much to reveal. The yet unknown…

The upcoming PANDA (anti-Proton ANnihilation at DArmstadt) experiment at FAIR (Facility for Anti-proton and Ion Research) offers unique possibilities for performing hyperon physics such as extraction of spin observables. Due to their…

Nuclear Experiment · Physics 2019-10-15 Jenny Regina , Walter Ikegami Andersson

We derive a method to improve particle identification (PID) at high transverse momentum ($p_T$) using the relativistic rise of the ionization energy loss ($rdE/dx$) when charged particles traverse the Time Projection Chamber (TPC) at STAR.…

This document presents the technical layout and the envisaged performance of the Electromagnetic Calorimeter (EMC) for the PANDA target spectrometer. The EMC has been designed to meet the physics goals of the PANDA experiment, which is…

Instrumentation and Detectors · 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

Particle IDentification (PID) is a central requirement of the experiments at the future EIC. Hadron PID at high momenta by RICH techniques requires the use of low density gaseous radiators, where the challenge is the limited length of the…

Here a preliminary study is presented concerning the detection of the normally unseen Drell-Yan fragments, possible in the PANDA experiment. To work as a multi-purpose apparatus, this experiment will record all the particles produced in the…

High Energy Physics - Phenomenology · Physics 2010-05-07 Andrea Bianconi

The barrel time-of-flight (TOF) detector for the PANDA experiment at FAIR in Darmstadt is planned as a scintillator tile hodoscope (SciTil) using 8000 small scintillator tiles. It will provide fast event timing for a software trigger in the…

Instrumentation and Detectors · Physics 2015-06-18 S. E. Brunner , L. Gruber , J. Marton , H. Orth , K. Suzuki

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 Multipurpose Detector (MPD) \cite{cite1.MPD_CDR} is designed to study of hot and dense baryonic matter in collisions of heavy ions over the atomic mass range 1--197 at the centre of mass energy up to $\sqrt{S_{NN}}$ = 11 GeV (for…

The correct identification of charged hadrons plays a crucial role in flavor-physics measurements. The final detector configurations at the proposed Future Circular Collider are yet to be determined and this study aims to contribute to this…

High Energy Physics - Experiment · Physics 2026-05-18 Anja Beck , Eluned Smith

High-efficiency and high-purity particle identification are fundamental requirements for the success of the Belle II experiment, whose main goal is to explore the new-physics scenarios in the CP-violating decays of the B mesons. To achieve…

High Energy Physics - Experiment · Physics 2018-11-13 Umberto Tamponi

Particle identification (PID) capabilities are studied by using the Time Projection Chamber (TPC) and a Time-Of-Flight (TOF) detector together at STAR. The identification capability of charged hadrons is greatly extended compared with that…

Nuclear Experiment · Physics 2011-07-19 M. Shao , O. Barannikova , X. Dong , Y. Fisyak , L. Ruan , P. Sorensen , Z. Xu

The ePIC detector is being designed as a general-purpose detector to deliver the full physics program of the Electron-Ion Collider (EIC) in BNL USA. Particle Identification (PID) plays a crucial role in the EIC physics program. Over a wide…

Instrumentation and Detectors · Physics 2025-01-07 Chandradoy Chatterjee

The Multi-Purpose Detector (MPD) is to be installed at the Nuclotron Ion Collider fAcility (NICA) of the Joint Institute for Nuclear Research (JINR). Its main goal is to study the phase diagram of the strongly interacting matter produced in…