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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

We present the design of the mechanical structure of the mini Beam-Beam detector, a subsystem of the Multi-Purpose Detector, soon to enter into operation at the Nuclotron based Ion Collider fAcility of the Joint Institute for Nuclear…

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

This submission will focus on advancements and advantages of Micro Pattern Gas Detector (MPGD) technologies and their applications to the construction of a dedicated Time Projection Chamber (TPC) that can serve as an excellent main tracker…

The Spin Physics Detector (SPD) experiment at the NICA collider in JINR aims to investigate the spin structure of nucleons and spin-related phenomena. The combination of the number of background processes, the event rate and conditions for…

Many current and future nuclear physics (NP) experiments across the United States have and are implementing micro-pattern gas detectors (MPGDs) to be used for tracking and PID purposes. MPGDs are capable of operating in high rate…

India-based Neutrino Observatory (INO) is a planned neutrino experiment to be build up in southern part of India.The INO observatory will host a 51 kton Iron Calorimeter (ICAL) detector to detect atmospheric neutrinos. Resistive Plate…

Instrumentation and Detectors · Physics 2014-11-24 Md. Naimuddin , Daljeet Kaur , Purnendu Kumar , Ankit Gaur , Praveen Kumar , Md. Hasbuddin , Swati Mishra , Ashok Kumar

The space-time picture of hadron formation in high-energy collisions with nuclear targets is still poorly known. The tests of hadron formation was suggested for the first stage of SPD running. They will require measuring charged pion and…

Instrumentation and Detectors · Physics 2024-08-22 R. Pandey

CLICdp, the CLIC detector and physics study, is an international collaboration presently composed of 23 institutions. The collaboration is addressing detector and physics issues for the future Compact Linear Collider (CLIC), a high-energy…

High Energy Physics - Experiment · Physics 2019-08-13 Aharon Levy

The LHC is not only the most powerful collider built to date but also the source of an intense beam of the most energetic neutrinos ever produced by humankind. After nearly 15 years of LHC operation, these neutrinos have been observed for…

High Energy Physics - Phenomenology · Physics 2025-01-14 Felix Kling

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

Heavy-ion collisions performed in the beam energy range accessible by the NICA collider facility are expected to produce systems of extreme net-baryon densities and can thus reach yet unexplored regions of the QCD phase diagram. Here, one…

Nuclear Theory · Physics 2016-09-21 Marlene Nahrgang , Christoph Herold

The CONNIE detector prototype is operating at a distance of 30 m from the core of a 3.8 GW$_{\rm th}$ nuclear reactor with the goal of establishing Charge-Coupled Devices (CCD) as a new technology for the detection of coherent elastic…

The 2015 nuclear physics long-range plan endorsed the realization of an Electron-Ion Collider (EIC) as the next large construction project after the completion of FRIB. With its high luminosity ( $> 10^{33} cm^{-2}s^{-1}$), wide kinematic…

Nuclear Experiment · Physics 2017-09-04 Salvatore Fazio

A simulation study of measurements of neutral current structure functions of the nucleon at the future high-energy and high-luminosity polarized electron-ion collider (EIC) is presented. A new series of $\gamma-Z$ interference structure…

Nuclear Experiment · Physics 2017-06-20 Y. X. Zhao , A. Deshpande , J. Huang , K. S. Kumar , S. Riordan

The facilities designed to study collisions of relativistic nuclei, such as the MPD at NICA (JINR), STAR at RHIC (BNL), ALICE, ATLAS and CMS at the LHC (CERN), are equipped with pairs of hadronic Zero Degree Calorimeters (ZDC) to detect…

Instrumentation and Detectors · Physics 2018-08-08 Uliana Dmitrieva , Igor Pshenichnov

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 MAGNEX large acceptance magnetic spectrometer is installed at the Laboratori Nazionali del Sud of the Istituto Nazionale di Fisica Nucleare (INFN-LNS) in Catania. In the past, MAGNEX experimental campaigns were performed using ion beams…

One proposed component of the upcoming Deep Underground Neutrino Experiment (DUNE) near detector complex is a multi-purpose, magnetized, gaseous argon time projection chamber: the Multi-Purpose Detector (MPD). We explore the new-physics…

High Energy Physics - Phenomenology · Physics 2020-03-18 Jeffrey M. Berryman , André de Gouvêa , Patrick J. Fox , Boris J. Kayser , Kevin J. Kelly , Jennifer L. Raaf

The Electron Ion Collider will have two interaction regions that can be instrumented with detectors. The first region will be instrumented as part of the project and needs to be capable of delivering the physics that has been outlined by…

Instrumentation and Detectors · Physics 2022-03-01 Douglas W. Higinbotham