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Antiproton--proton annihilation into light neutral mesons in the few GeV energy domain is investigated in view of a global description of the existing data and predictions for future experiments at PANDA, FAIR. An effective meson model…

High Energy Physics - Phenomenology · Physics 2017-09-13 Ying Wang , Yury M. Bystritskiy , Azad I. Ahmadov , Egle Tomasi Gustafsson

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 Compressed Baryonic Matter (CBM) experiment at the future Facility for Antiproton and Ion Research (FAIR) in Darmstadt is designed to investigate the properties of high-density QCD matter with multi-differential measurements of hadrons…

Nuclear Experiment · Physics 2021-06-01 Anna Senger , Peter Senger

The Facility for Antiproton and Ion Research (FAIR) in Darmstadt will provide unique research opportunities for the investigation of fundamental open questions related to nuclear physics and astrophysics, including the exploration of QCD…

Nuclear Experiment · Physics 2020-05-08 Peter Senger

Spectroscopy of Lambda hypernuclei has recently become one of the most valuable tools for the experimental investigation of strangeness nuclear physics. Several new approached are being pursued currently: In Mainz, the Microtron MAMI has…

Nuclear Experiment · Physics 2007-11-19 Patrick Achenbach

Fermilab operates the world's most intense antiproton source. Recently proposed experiments can use those antiprotons either parasitically during Tevatron Collider running or after the Tevatron Collider finishes in about 2011. For example,…

High Energy Physics - Phenomenology · Physics 2010-08-02 Daniel M. Kaplan

We introduce the polymer analysis and discovery array (PANDA), an automated system for high-throughput electrodeposition and functional characterization of polymer films. The PANDA is a custom, modular, and low-cost system based on a CNC…

Fermilab operates the world's most intense antiproton source. Newly proposed experiments can use those antiprotons either parasitically during Tevatron Collider running or after the Tevatron Collider finishes. For example, the annihilation…

High Energy Physics - Experiment · Physics 2017-08-23 Daniel M. Kaplan

Proton radiography is used in various high-energy-density (HED) plasma experiments. In this paper, we describe a Monte Carlo and ray-tracing simulation tool called MPRAD that can be used for modeling the deflection of proton beams in…

Plasma Physics · Physics 2020-01-08 Yingchao Lu , Hui Li , Kirk A. Flippo , Kwyntero Kelso , Andy Liao , Shengtai Li , Edison Liang

We study the formation of single- and double-$\Lambda$ hypernuclei in antiproton-induced reactions relevant for the forthcoming PANDA experiment at FAIR. We use the Giessen Boltzmann-Uehling-Uhlenbeck (GiBUU) transport model with…

Nuclear Theory · Physics 2015-06-03 T. Gaitanos , A. B. Larionov , H. Lenske , U. Mosel

The future Facility for Anti-proton and Ion Research (FAIR), currently in construction in Darmstadt, Germany, is one of the largest research projects worldwide. The Compressed Baryonic Matter (CBM) experiment is one of the main pillars at…

Instrumentation and Detectors · Physics 2021-02-03 Qiunan Zhang , Ingo Deppner , Nobert Herrmann , Yi Wang

This document illustrates the technical layout and the expected performance of the Micro Vertex Detector (MVD) of the PANDA experiment. The MVD will detect charged particles as close as possible to the interaction zone. Design criteria and…

Instrumentation and Detectors · Physics 2012-08-13 PANDA Collaboration , W. Erni , I. Keshelashvili , B. Krusche , M. Steinacher , Y. Heng , Z. Liu , H. Liu , X. Shen , Q. Wang , H. Xu , M. Albrecht , J. Becker , K. Eickel , F. Feldbauer , M. Fink , P. Friedel , F. H. Heinsius , T. Held , H. Koch , B. Kopf , M. Leyhe , C. Motzko , M. Pelizäus , J. Pychy , B. Roth , T. Schröder , J. Schulze , M. Steinke , T. Trifterer , U. Wiedner , J. Zhong , R. Beck , M. Becker , S. Bianco , K. -Th. Brinkmann , C. Hammann , F. Hinterberger , R. Jäkel , D. Kaiser , R. Kliemt , K. Koop , C. Schmidt , R. Schnell , U. Thoma , P. Vlasov , C. Wendel , A. Winnebeck , Th. Würschig , H. -G. Zaunick , A. Bianconi , M. Bragadireanu , M. Caprini , M. Ciubancan , D. Pantea , P. -D Tarta , M. De Napoli , F. Giacoppo , E. Rapisarda , C. Sfienti , T. Fiutowski , N. Idzik , B. Mindur , D. Przyborowski , K. Swientek , E. Bialkowski , A. Budzanowski , B. Czech , S. Kliczewski , A. Kozela , P. Kulessa , P. Lebiedowicz , K. Malgorzata , K. Pysz , W. Schäfer , R. Siudak , A. Szczurek , P. Brandys , T. Czyzewski , W. Czyzycki , M. Domagala , M. Hawryluk , G. Filo , D. Kwiatkowski , E. Lisowski , F. Lisowski , W. Bardan , D. Gil , B. Kamys , St. Kistryn , K. Korcyl , W. Krzemieñ , A. Magiera , P. Moskal , Z. Rudy , P. Salabura , J. Smyrski , A. Wroñska , M. Al-Turany , R. Arora , I. Augustin , H. Deppe , D. Dutta , H. Flemming , K. Götzen , G. Hohler , R. Karabowicz , D. Lehmann , B. Lewandowski , J. Lühning , F. Maas , H. Orth , K. Peters , T. Saito , G. Schepers , C. J. Schmidt , L. Schmitt , C. Schwarz , J. Schwiening , B. Voss , P. Wieczorek , A. Wilms , V. M. Abazov , G. D. Alexeev , V. 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. I. Lobanov , Yu. Yu. Lobanov , A. F. Makarov , L. V. Malinina , V. L. Malyshev , G. A. Mustafaev , A. G. 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 , 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. Vodopyanov , S. A. Zaporozhets , N. I. Zhuravlev , A. G. Zorin , D. Branford , D. Glazier , D. Watts , P. Woods , A. Britting , W. Eyrich , A. Lehmann , F. Uhlig , S. Dobbs , Z. Metreveli , K. Seth , B. Tann , A. Tomaradze , D. Bettoni , V. Carassiti , P. Dalpiaz , A. Drago , E. Fioravanti , I. Garzia , M. Negrini , M. Savriè , G. Stancari , B. Dulach , P. Gianotti , C. Guaraldo , V. Lucherini , E. Pace , A. Bersani , M. Macri , M. Marinelli , R. F. Parodi , V. Dormenev , P. Drexler , M. Düren , T. Eisner , K. Foehl , A. Hayrapetyan , P. Koch , B. Krïoch , W. Kühn , S. Lange , Y. Liang , M. Liu , O. Merle , V. Metag , M. Moritz , M. Nanova , R. Novotny , B. Spruck , H. Stenzel , C. Strackbein , M. Thiel , Q. Wang , T. Clarkson , C. Euan , G. Hill , M. Hoek , D. Ireland , R. Kaiser , T. Keri , I. Lehmann , K. Livingston , P. Lumsden , D. MacGregor , B. McKinnon , R. Montgomery , M. Murray , D. Protopopescu , G. Rosner , B. Seitz , G. Yang , M. Babai , A. K. Biegun , A. Glazenborg-Kluttig , E. Guliyev , V. S. Jothi , M. Kavatsyuk , P. Lemmens , H. Löhner , J. Messchendorp , T. Poelman , H. Smit , J. C. van der Weele , H. Sohlbach , M. Büscher , R. Dosdall , R. Dzhygadlo , S. Esch , A. Gillitzer , F. Goldenbaum , D. Grunwald , V. Jha , G. Kemmerling , H. Kleines , A. Lehrach , R. Maier , M. Mertens , H. Ohm , D. L. Pohl , D. Prasuhn , T. Randriamalala , J. Ritman , M. Roeder , G. Sterzenbach , T. Stockmanns , P. Wintz , P. Wüstner , H. Xu , J. Kisiel , S. Li , Z. Li , Z. Sun , H. Xu , K. Fissum , K. Hansen , L. Isaksson , M. Lundin , B. Schröder , P. Achenbach , A. Denig , M. Distler , M. Fritsch , D. Kangh , A. Karavdina , W. Lauth , M. Michel , M. C. Mora Espi , J. Pochodzalla , S. Sanchez , A. Sanchez-Lorente , C. Sfienti , T. Weber , 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 , R. Varma , B. Ketzer , I. Konorov , A. Mann , S. Neubert , S. Paul , M. Vandenbroucke , Q. Zhang , A. Khoukaz , T. Rausmann , A. Täschner , J. Wessels , E. Baldin , K. Kotov , S. Peleganchuk , Yu. Tikhonov , T. Hennino , M. Imre , R. Kunne , C. Le Galliard , J. P. Le Normand , D. Marchand , A. Maroni , S. Ong , J. Pouthas , B. Ramstein , P. Rosier , M. Sudol , C. Theneau , E. Tomasi-Gustafsson , J. Van de Wiele , T. Zerguerras , G. Boca , A. Braghieri , S. Costanza , A. Fontana , P. Genova , L. Lavezzi , P. Montagna , A. Rotondi , V. Buda , V. V. Abramov , A. M. Davidenko , A. A. Derevschikov , Y. M. Goncharenko , V. N. Grishin , V. A. Kachanov , D. A. Konstantinov , V. A. Kormilitsin , 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 , S. Belostotski , G. Gavrilov , A. Itzotov , A. Kisselev , P. Kravchenko , S. Manaenkov , O. Miklukho , Y. Naryshkin , D. Veretennikov , V. Vikhrov , A. Zhadanov , T. Bäck , B. Cederwall , C. Bargholtz , L. Gerén , P. E. Tegnér , P. Thørngren , K. M. von Würtemberg , L. Fava , D. Alberto , A. Amoroso , M. P. Bussa , L. Busso , F. De Mori , M. Destefanis , L. Ferrero , M. Greco , T. Kugathasan , M. Maggiora , S. Marcello , S. Sosio , S. Spataro , D. Calvo , S. Coli , P. De Remigis , A. Filippi , G. Giraudo , S. Lusso , G. Mazza , M. Mignone , A. Rivetti , R. Wheadon , L. Zotti , O. Morra , F. Iazzi , A. Lavagno , P. Quarati , K. Szymanska , R. Birsa , F. Bradamante , A. Bressan , A. Martin , H. Clement , B. Galnander , H. Calén , K. Fransson , T. Johansson , A. Kupsc , P. Marciniewski , E. Thomé , M. Wolke , J. Zlomanczuk , J. Díaz , A. Ortiz , P. Buda , K. Dmowski , R. Korzeniewski , D. Przemyslaw , B. Slowinski , S. Borsuk , A. Chlopik , Z. Guzik , J. Kopec , T. Kozlowski , D. Melnychuk , M. Plominski , J. Szewinski , K. Traczyk , B. Zwieglinski , P. Bühler , A. Gruber , P. Kienle , J. Marton , E. Widmann , J. Zmeskal

The FAIR[1] facility is an international accelerator centre for research with ion and antiproton beams. It is being built at Darmstadt, Germany as an extension to the current GSI research institute. One major part of the facility will be…

The Compressed Baryonic Matter (CBM) experiment is a next-generation heavy-ion experiment under development at the future FAIR facility in Darmstadt, Germany. It is designed to explore the QCD phase diagram at high net-baryon densities with…

Instrumentation and Detectors · Physics 2025-06-26 Maksym Teklishyn

A new generation of high-resolution hypernuclear gamma$-spectroscopy experiments with high-purity germanium detectors (HPGe) are presently designed at the FINUDA spectrometer at DAPhiNE, the Frascati phi-factory, and at PANDA, the…

We report on the design and characterization of an antiproton deceleration beamline, based on a pulsed drift tube, for the PUMA experiment at the Antimatter Factory at CERN. The design has been tailored to high-voltage (100 kV) and…

Instrumentation and Detectors · Physics 2024-06-04 J. Fischer , A. Schmidt , N. Azaryan , F. Butin , J. Ferreira Somoza , A. Husson , C. Klink , A. Obertelli , M. Schlaich , A. Sinturel , N. Thaus , F. Wienholtz

Fermilab operates the world's most intense antiproton source. Newly proposed experiments can use those antiprotons either parasitically during Tevatron Collider running or after the Tevatron Collider finishes in about 2010. In particular,…

High Energy Physics - Experiment · Physics 2008-10-19 Daniel M. Kaplan

The Reactions with Relativistic Radioactive Beams (R$^3$B) collaboration of the Facility for Antiproton and Ion Research (FAIR) in Darmstadt, Germany, has constructed an experimental setup to perform fundamental studies of nuclear matter,…

Instrumentation and Detectors · Physics 2023-07-19 M. Xarepe , T. Aumann , A. Blanco , A. Corsi , D. Galaviz , H. Johansson , S. Linev , B. Löher , L. Lopes , J. Michel , V. Panin , D. Rossi , J. Saraiva , H. Törnqvist , M. Traxler

India is a founder-member country to participate in the construction of the international multipurpose accelerator facility called the Facility for Antiproton and Ion Research (FAIR) at Darmstadt, Germany. Bose Institute, Kolkata, has been…

High Energy Physics - Experiment · Physics 2025-05-01 Saikat Biswas

The antiProton Unstable Matter Annihilation experiment (PUMA) at CERN aims at investigating the nucleon composition in the matter density tail of radioactive as well as stable isotopes by use of low-energy antiproton-nucleon annihilation…

Instrumentation and Detectors · Physics 2023-11-29 M. Schlaich , J. Fischer , P. Fischer , C. Klink , A. Obertelli , A. Schmidt , L. Schweikhard , F. Wienholtz