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A time projection chamber (TPC) is a strong candidate for the central tracker of the international linear collider (ILC) experiment and we have been conducting a series of cosmic ray experiments under a magnetic field up to 4 T, using a…

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…

The PANDA collaboration intends to build a state-of-the-art detector to study the physics of antiproton annihilation in the charm mass region at the future FAIR facility at GSI, Darmstadt. One major part of the PANDA detector is the straw…

Nuclear Experiment · Physics 2008-11-26 Andrey Sokolov , James Ritman , Peter Wintz

The dual-phase xenon time projection chamber (TPC) is a leading detector technology in rare event searches for dark matter and neutrino physics. The success of this type of detector technology relies on its capability to detect both primary…

Instrumentation and Detectors · Physics 2022-02-16 Yuehuan Wei , Jianyang Qi , Evan Shockley , Haiwen Xu , Kaixuan Ni

The Time Projection Chamber (TPC) has been recognized as a potentially powerful detector for the search of WIMPs by measuring the directions of nuclear recoils, in which the most convincing signature of WIMPs, caused by the Earth's motion…

Gas Electron Multiplier (GEM) is one of the mostly used gaseous detectors in the High Energy Physics (HEP) experiments. GEMs are widely used as tracking devices due to their high-rate handling capability and good position resolution. An…

High Energy Physics - Experiment · Physics 2024-01-23 S. Mandal , S. Chatterjee , A. Sen , S. Gope , S. Dhani , A. C. Hegde , M. Chatterjee , S. Das , S. Biswas

The upgrade of the ALICE TPC will allow the experiment to cope with the high interaction rates foreseen for the forthcoming Run 3 and Run 4 at the CERN LHC. In this article, we describe the design of new readout chambers and front-end…

Instrumentation and Detectors · Physics 2021-03-26 J. Adolfsson , M. Ahmed , S. Aiola , J. Alme , T. Alt , W. Amend , F. Anastasopoulos , C. Andrei , M. Angelsmark , V. Anguelov , A. Anjam , H. Appelshäuser , V. Aprodu , O. Arnold , M. Arslandok , D. Baitinger , M. Ball , G. G. Barnaföldi , E. Bartsch , P. Becht , R. Bellwied , A. Berdnikova , M. Berger , N. Bialas , P. Bialas , S. Biswas , B. Blidaru , L. Boldizsár , L. Bratrud , P. Braun-Munzinger , M. Bregant , C. L. Britton , S. Brucker , E. J. Brücken , H. Büsching , R. Soto Camacho , A. L. Campos , G. Caragheorgheopol , D. D. Carvalho , A. J. Castro , P. Chatzidaki , P. Christiansen , L. G. Clonts , T. M. Cormier , A. L. D. Couto , H. G. A. Cubas , A. Deisting , P. Dhankher , S. Dittrich , V. Duta , R. Ehlers , M. Engel , M. N. Ericson , N. B. Ezell , L. Fabbietti , F. Flor , G. Föhner , U. Frankenfeld , E. Futo , J. J. Gaardhøje , M. G. Munhoz , C. Garabatos , P. Gasik , T. Geiger , Á. Gera , P. Glässel , D. J. Q. Goh , O. Grachov , A. Grein , M. Gul , T. Gunji , M. Habib , H. Hamagaki , G. Hamar , J. C. Hansen , A. Harlenderova , J. W. Harris , S. Hassan , P. Hauer , S. Hayashi , S. T. Heckel , J. Hehner , J. K. Heino , E. Hellbär , H. Helstrup , A. Herghelegiu , L. Hernandes da Costa Porto , R. A. Hernandez , H. D. Hernandez Herrera , T. Herold , T. E. Hilden , B. Hohlweger , S. Hornung , C. Hughes , S. Hummel , M. Ivanov , J. Jung , M. Jung , D. Just , E. Kangasaho , L. Karayan , B. Ketzer , S. Kirsch , M. Kleiner , T. Klemenz , S. Klewin , A. G. Knospe , E. Koskinen , M. Kowalski , L. Kreis , M. Krüger , N. Kupfer , R. Lang , L. Lautner , M. Lesch , Y. Lesenechal , F. Liebske , C. Lippmann , V. Litichevskyi , M. Ljunggren , W. J. Llope , S. Mahmood , T. Mahmoud , R. D. Majka , C. Markert , J. Martinez , T. A. Martins , S. Masciocchi , A. Mathis , O. Matonoha , Y. Matsuyama , A. Matyja , M. Meres , D. L. Mihaylov , D. Miśkowiec , T. Mittelstaedt , L. S. Montali , D. M. Moraes , C. Mordasini , T. Morhardt , S. Muley , J. Mulligan , R. H. Munzer , H. Murakami , K. Münning , A. Nassirpour , H. Natal da Luz , C. Nattrass , R. A. Negrao De Oliveira , H. G. Neves , B. S. Nielsen , W. A. V. Noije , M. Ogino , A. C. Oliveira Da Silva , A. Oskarsson , J. Ottnad , K. Oyama , A. Önnerstad , L. Österman , A. A. Pabon , Y. Pachmayer , G. Paić , J. Parkkila , S. Pathak , R. N. Patra , V. Peskov , M. Petris , M. Petrovici , M. Planinic , F. Pompei , L. Prodan , A. Radu , L. Radulescu , J. Rak , J. Rasson , V. Ratza , K. F. Read , A. Rehman , R. Renfordt , K. Røed , D. Röhrich , E. Rubio , T. Rudzki , A. Rusu , M. Saleh , B. C. S. Sanches , J. Schambach , S. Scheid , C. Schmidt , A. Schmier , H. Schulte , K. Schweda , D. Sekihata , N. Shimizu , S. Siebig , R. W. D. Silva , D. Silvermyr , D. Simpson , B. Sitar , N. Smirnov , T. Snellman , H. K. Soltveit , S. P. Sorensen , F. Sozzi , J. Stachel , A. Szabo , L. Šerkšnytė , Y. Takeuchi , G. Tambave , Y. Tanaka , K. Terasaki , R. J. Turpeinen , K. Ullaland , B. Ulukutlu , E. Umaka , A. Utrobicic , D. Varga , A. Vargas , M. Vargyas , R. Varma , O. Vazquez Rueda , A. Velure , S. Vereschagin , S. Vergara Limón , L. Vergara Urrutia , O. Vorbach , B. Voss , D. Vranic , R. J. Warmack , T. O. Weber , C. Weidlich , J. Wiechula , B. Windelband , S. Winkler , W. Witt

Time Projection Chamber (TPC) is one of the main tracking systems for many current and future collider experiments at RHIC and LHC. It has a capability to measure the space points of charged tracks for good momentum resolution as well as…

Instrumentation and Detectors · Physics 2019-12-30 K. Dehmelt , P. Garg , T. K. Hemmick , A. Milov , E. Shulga , V. Zakharov

The Time Projection Chamber (TPC) is an ideal candidate to finely study the charged particle ionization in a gaseous medium. Large volumes TPCs can be read out with a suitable number of channels offering a complete 3D reconstruction of an…

In experiments searching for rare signals, background events from the detector itself are some of the major factors limiting search sensitivity.Screening for ultra-low radioactive detector materials is becoming ever more essential. We…

Instrumentation and Detectors · Physics 2021-12-24 Haiyan Du , Chengbo Du , Karl Giboni , Ke Han , Shengming He , Liqiang Liu , Yue Meng , Shaobo Wang , Tao Zhang , Li Zhao , Jifang Zhou

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 ALICE experiment at the Large Hadron Collider at CERN is upgrading its central tracking detector, the Time Projection Chamber (TPC). The installation is foreseen during the second long shutdown of the Large Hadron Collider. The upgrade…

Instrumentation and Detectors · Physics 2018-11-20 Jens Erik Brücken , Timo Eero Hildén

A fundamental limit to the application of Time Projection Chambers (TPCs) in high-rate experiments is the accumulation of slowly drifting ions in the active gas volume, which compromises the homogeneity of the drift field and hence the…

Instrumentation and Detectors · Physics 2012-09-05 F. V. Böhmer , M. Ball , S. Dørheim , C. Höppner , B. Ketzer , I. Konorov , S. Neubert , S. Paul , J. Rauch , M. Vandenbroucke

The Resistive Plate Chambers (RPC) detector of the CMS experiment at the LHC proton collider (CERN, Switzerland) will employ an online gas analysis and monitoring system of the freon-based gas mixture used. We give an overview of the CMS…

We successfully operated a novel kind of LAr Time Projection Chamber based on a Large Electron Multiplier (LEM) readout system. The prototype, of about 3 liters active volume, is operated in liquid-vapour (double) phase pure Ar. The…

Instrumentation and Detectors · Physics 2008-11-21 A. Badertscher , L. Knecht , M. Laffranchi , A. Marchionni , G. Natterer , P. Otiougova , F. Resnati , A. Rubbia

Two cylindrical forward TPC detectors are described which were constructed to extend the phase space coverage of the STAR experiment to the region 2.5 < |\eta| < 4.0. For optimal use of the available space and in order to cope with the high…

The sPHENIX Time Projection Chamber Outer Tracker (TPOT) is a Micromegas based detector. It is a part of the sPHENIX experiment that aims to facilitate the calibration of the Time Projection Chamber, in particular the correction of the…

An upgrade of the near detector of the T2K long baseline neutrino oscillation experiment is currently being conducted. This upgrade will include two new Time Projection Chambers, each equipped with 16 charge readout resistive Micromegas…

Resistive Plate Chamber (RPC) is a gaseous detector, known for its good spatial resolution and excellent time resolution. Due to its fast response and excellent time resolution, it is used for both triggering and timing purpose. But the…

Instrumentation and Detectors · Physics 2022-10-26 Jaydeep Datta , Nayana Majumdar , Supratik Mukhopadhyay , Sandip Sarkar
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