English
Related papers

Related papers: The PANDA Barrel DIRC

200 papers

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 PHENIX collaboration has designed a conceptually new Hadron Blind Detector (HBD) for electron identification in high density hadron environment. The HBD will identify low momentum electron-positron pairs to reduce the combinatorial…

Nuclear Experiment · Physics 2009-11-11 A. Milov

We review recent Z^0 physics results from SLD that use the Cherenkov Ring Imaging Detector for charged particle identification. The performance of the detector and likelihood method are described briefly. Several hadronization measurements…

High Energy Physics - Experiment · Physics 2008-11-26 D. Muller , representing the SLD Collaboration

We present a machine-learning-based particle-identification study for the proximity-focusing Ring Imaging Cherenkov (pfRICH) detector of the ePIC experiment at the Electron-Ion Collider. Operating in the backward region ($-3.5 \lesssim \eta…

Instrumentation and Detectors · Physics 2025-12-30 D. H. Dongwi , C. -J. Naïm , L. Rhode , A. Deshpande

Imaging Cherenkov detectors are crucial for particle identification (PID) in nuclear and particle physics experiments. Fast reconstruction algorithms are essential for near real-time alignment, calibration, data quality control, and…

Instrumentation and Detectors · Physics 2024-07-11 Cristiano Fanelli , James Giroux , Justin Stevens

The integration of Deep Learning (DL) into experimental nuclear and particle physics has driven significant progress in simulation and reconstruction workflows. However, traditional simulation frameworks such as Geant4 remain…

Instrumentation and Detectors · Physics 2025-04-29 James Giroux , Michael Martinez , Cristiano Fanelli

Liquid argon time projection chambers (LArTPCs) provide dense, high-fidelity 3D measurements of particle interactions and underpin current and future neutrino and rare-event experiments. Physics reconstruction typically relies on complex…

High Energy Physics - Experiment · Physics 2025-12-02 Samuel Young , Kazuhiro Terao

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

We have developed a new type of particle identification device, called an Aerogel Ring Imaging Cherenkov (ARICH) counter, for the Belle II experiment. It uses silica aerogel tiles as Cherenkov radiators. For detection of Cherenkov photons,…

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 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…

Nearby Photo-Dissociation Regions (PDRs), where the gas and dust are heated by the far UV-irradiation emitted from stars, are ideal templates to study the main stellar feedback processes. With this study we aim to probe the detailed…

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

The Crystal Barrel is an electromagnetic calorimeter consisting of 1380 CsI(Tl) scintillators, and is currently installed at the CBELSA/TAPS experiment where it is used to detect decay products from photoproduction of mesons. The readout of…

The PANDA (anti-Proton ANnihilation at DArmstadt) experiment at the Facility for Anti-proton and Ion Research is going to study strong interactions at the scale at which quarks are confined to form hadrons. A continuous beam of antiproton,…

High Energy Physics - Experiment · Physics 2022-12-01 Adeel Akram , Xiangyang Ju

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 exclusive charmonium production process in $\bar{p}p$ annihilation with an associated $\pi^0$ meson $\bar{p}p\to J/\psi\pi^0$ is studied in the framework of QCD collinear factorization. The feasibility of measuring this reaction through…

Nuclear Experiment · Physics 2017-02-22 PANDA Collaboration , B. Singh , W. Erni , B. Krusche , M. Steinacher , N. Walford , H. Liu , Z. Liu , B. Liu , X. Shen , C. Wang , J. Zhao , M. Albrecht , T. Erlen , M. Fink , F. H. Heinsius , T. Held , T. Holtmann , S. Jasper , I. Keshk , H. Koch , B. Kopf , M. Kuhlmann , M. Kümmel , S. Leiber , M. Mikirtychyants , P. Musiol , A. Mustafa , M. Pelizäus , J. Pychy , M. Richter , C. Schnier , T. Schröder , C. Sowa , M. Steinke , T. Triffterer , U. Wiedner , M. Ball , R. Beck , C. Hammann , B. Ketzer , M. Kube , P. Mahlberg , M. Rossbach , C. Schmidt , R. Schmitz , U. Thoma , M. Urban , D. Walther , C. Wendel , A. Wilson , A. Bianconi , M. Bragadireanu , M. Caprini , D. Pantea , B. Patel , W. Czyzycki , M. Domagala , G. Filo , J. Jaworowski , M. Krawczyk , E. Lisowski , F. Lisowski , M. Michałek , P. Poznański , J. Płażek , K. Korcyl , A. Kozela , P. Kulessa , P. Lebiedowicz , K. Pysz , W. Schäfer , A. Szczurek , T. Fiutowski , M. Idzik , B. Mindur , D. Przyborowski , K. Swientek , J. Biernat , B. Kamys , S. Kistryn , G. Korcyl , W. Krzemien , A. Magiera , P. Moskal , A. Pyszniak , Z. Rudy , P. Salabura , J. Smyrski , P. Strzempek , A. Wronska , I. Augustin , R. Böhm , I. Lehmann , D. Nicmorus Marinescu , L. Schmitt , V. Varentsov , M. Al-Turany , A. Belias , H. Deppe , N. Divani Veis , R. Dzhygadlo , A. Ehret , H. Flemming , A. Gerhardt , K. Götzen , A. Gromliuk , L. Gruber , R. Karabowicz , R. Kliemt , M. Krebs , U. Kurilla , D. Lehmann , S. Löchner , J. Lühning , U. Lynen , H. Orth , M. Patsyuk , K. Peters , T. Saito , G. Schepers , C. J. Schmidt , C. Schwarz , J. Schwiening , A. Täschner , M. Traxler , C. Ugur , B. Voss , P. Wieczorek , A. Wilms , M. Zühlsdorf , V. Abazov , G. Alexeev , V. A. Arefiev , V. Astakhov , M. Yu. Barabanov , B. V. Batyunya , Y. Davydov , V. Kh. Dodokhov , A. Efremov , A. Fechtchenko , A. G. Fedunov , A. Galoyan , S. Grigoryan , E. K. Koshurnikov , Y. Yu. Lobanov , V. I. Lobanov , A. F. Makarov , L. V. Malinina , V. Malyshev , A. G. Olshevskiy , E. Perevalova , A. A. Piskun , T. Pocheptsov , G. Pontecorvo , V. Rodionov , Y. Rogov , R. Salmin , A. Samartsev , M. G. Sapozhnikov , G. Shabratova , N. B. Skachkov , A. N. Skachkova , E. A. Strokovsky , M. Suleimanov , R. Teshev , V. Tokmenin , V. Uzhinsky , A. Vodopianov , S. A. Zaporozhets , N. I. Zhuravlev , A. Zinchenko , A. G. Zorin , D. Branford , D. Glazier , D. Watts , M. Böhm , A. Britting , W. Eyrich , A. Lehmann , M. Pfaffinger , F. Uhlig , S. Dobbs , K. Seth , A. Tomaradze , T. Xiao , D. Bettoni , V. Carassiti , A. Cotta Ramusino , P. Dalpiaz , A. Drago , E. Fioravanti , I. Garzia , M. Savrie , V. Akishina , I. Kisel , G. Kozlov , M. Pugach , M. Zyzak , P. Gianotti , C. Guaraldo , V. Lucherini , A. Bersani , G. Bracco , M. Macri , R. F. Parodi , K. Biguenko , K. T. Brinkmann , V. Di Pietro , S. Diehl , V. Dormenev , P. Drexler , M. Düren , E. Etzelmüller , M. Galuska , E. Gutz , C. Hahn , A. Hayrapetyan , M. Kesselkaul , W. Kühn , T. Kuske , J. S. Lange , Y. Liang , V. Metag , M. Moritz , M. Nanova , S. Nazarenko , R. Novotny , T. Quagli , S. Reiter , A. Riccardi , J. Rieke , C. Rosenbaum , M. Schmidt , R. Schnell , H. Stenzel , U. Thöring , T. Ullrich , M. N. Wagner , T. Wasem , B. Wohlfahrt , H. G. Zaunick , E. Tomasi-Gustafsson , D. Ireland , G. Rosner , B. Seitz , P. N. Deepak , A. Kulkarni , A. Apostolou , M. Babai , M. Kavatsyuk , P. J. Lemmens , M. Lindemulder , H. Loehner , J. Messchendorp , P. Schakel , H. Smit , M. Tiemens , J. C. van der Weele , R. Veenstra , S. Vejdani , K. Dutta , K. Kalita , A. Kumar , A. Roy , H. Sohlbach , M. Bai , L. Bianchi , M. Büscher , L. Cao , A. Cebulla , R. Dosdall , A. Gillitzer , F. Goldenbaum , D. Grunwald , A. Herten , Q. Hu , G. Kemmerling , H. Kleines , A. Lai , A. Lehrach , R. Nellen , H. Ohm , S. Orfanitski , D. Prasuhn , E. Prencipe , J. Pütz , J. Ritman , S. Schadmand , T. Sefzick , V. Serdyuk , G. Sterzenbach , T. Stockmanns , P. Wintz , P. Wüstner , H. Xu , A. Zambanini , S. Li , Z. Li , Z. Sun , H. Xu , V. Rigato , L. Isaksson , P. Achenbach , O. Corell , A. Denig , M. Distler , M. Hoek , A. Karavdina , W. Lauth , Z. Liu , H. Merkel , U. Müller , J. Pochodzalla , S. Sanchez , S. Schlimme , C. Sfienti , M. Thiel , H. Ahmadi , S. Ahmed , S. Bleser , L. Capozza , M. Cardinali , A. Dbeyssi , M. Deiseroth , F. Feldbauer , M. Fritsch , B. Fröhlich , D. Kang , D. Khaneft , R. Klasen , H. H. Leithoff , D. Lin , F. Maas , S. Maldaner , M. Martínez , M. Michel , M. C. Mora Espí , C. Morales Morales , C. Motzko , F. Nerling , O. Noll , S. Pflüger , A. Pitka , D. Rodríguez Piñeiro , A. Sanchez-Lorente , M. Steinen , R. Valente , T. Weber , M. Zambrana , I. Zimmermann , A. Fedorov , M. Korjik , O. Missevitch , A. Boukharov , O. Malyshev , I. Marishev , V. Balanutsa , P. Balanutsa , V. Chernetsky , A. Demekhin , A. Dolgolenko , P. Fedorets , A. Gerasimov , V. Goryachev , V. Chandratre , V. Datar , D. Dutta , V. Jha , H. Kumawat , A. K. Mohanty , A. Parmar , B. Roy , G. Sonika , C. Fritzsch , S. Grieser , A. K. Hergemöller , B. Hetz , N. Hüsken , A. Khoukaz , J. P. Wessels , K. Khosonthongkee , C. Kobdaj , A. Limphirat , P. Srisawad , Y. Yan , A. Yu. Barnyakov , M. Barnyakov , K. Beloborodov , V. E. Blinov , V. S. Bobrovnikov , I. A. Kuyanov , K. Martin , A. P. Onuchin , S. Serednyakov , A. Sokolov , Y. Tikhonov , A. E. Blinov , S. Kononov , E. A. Kravchenko , E. Atomssa , R. Kunne , B. Ma , D. Marchand , B. Ramstein , J. van de Wiele , Y. Wang , G. Boca , S. Costanza , P. Genova , P. Montagna , A. Rotondi , V. Abramov , N. Belikov , S. Bukreeva , A. Davidenko , A. Derevschikov , Y. Goncharenko , V. Grishin , V. Kachanov , V. Kormilitsin , A. Levin , Y. Melnik , N. Minaev , V. Mochalov , D. Morozov , L. Nogach , S. Poslavskiy , A. Ryazantsev , S. Ryzhikov , P. Semenov , I. Shein , A. Uzunian , A. Vasiliev , A. Yakutin , U. Roy , B. Yabsley , S. Belostotski , G. Gavrilov , A. Izotov , S. Manaenkov , O. Miklukho , D. Veretennikov , A. Zhdanov , T. Bäck , B. Cederwall , K. Makonyi , M. Preston , P. E. Tegner , D. Wölbing , A. K. Rai , S. Godre , D. Calvo , S. Coli , P. De Remigis , A. Filippi , G. Giraudo , S. Lusso , G. Mazza , M. Mignone , A. Rivetti , R. Wheadon , A. Amoroso , M. P. Bussa , L. Busso , F. De Mori , M. Destefanis , L. Fava , L. Ferrero , M. Greco , J. Hu , L. Lavezzi , M. Maggiora , G. Maniscalco , S. Marcello , S. Sosio , S. Spataro , F. Balestra , F. Iazzi , R. Introzzi , A. Lavagno , J. Olave , R. Birsa , F. Bradamante , A. Bressan , A. Martin , H. Calen , W. Ikegami Andersson , T. Johansson , A. Kupsc , P. Marciniewski , M. Papenbrock , J. Pettersson , K. Schönning , M. Wolke , B. Galnander , J. Diaz , V. Pothodi Chackara , A. Chlopik , G. Kesik , D. Melnychuk , B. Slowinski , A. Trzcinski , M. Wojciechowski , S. Wronka , B. Zwieglinski , P. Bühler , J. Marton , D. Steinschaden , K. Suzuki , E. Widmann , J. Zmeskal , K. M. Semenov-Tian-Shansky

A Hadron Blind Detector (HBD) is being developed for the PHENIX experiment at RHIC. It consists of a Cherenkov radiator operated with pure CF4 directly coupled in a windowless configuration to a triple-GEM detector element with a CsI…

High performance calorimetry conducted at future hadron colliders, such as the FCC-hh, poses a significant challenge for applying current detector technologies due to unprecedented beam luminosities and radiation fields. Solutions include…