English
Related papers

Related papers: Triple GEM Detectors for the Forward Tracker in ST…

200 papers

A large Time Projection Chamber is the main device for tracking and charged-particle identification in the ALICE experiment at the CERN LHC. After the second long shutdown in 2019/20, the LHC will deliver Pb beams colliding at an…

Instrumentation and Detectors · Physics 2018-07-16 M. M. Aggarwal , Z. Ahammed , S. Aiola , J. Alme , T. Alt , W. Amend , A. Andronic , V. Anguelov , H. Appelshäuser , M. Arslandok , R. Averbeck , M. Ball , G. G. Barnaföldi , E. Bartsch , R. Bellwied , G. Bencedi , M. Berger , N. Bialas , P. Bialas , L. Bianchi , S. Biswas , L. Boldizsár , L. Bratrud , P. Braun-Munzinger , M. Bregant , C. L. Britton , E. J. Brucken , H. Caines , A. J. Castro , S. Chattopadhyay , P. Christiansen , L. G. Clonts , T. M. Cormier , S. Das , S. Dash , A. Deisting , S. Dittrich , A. K. Dubey , R. Ehlers , M. Engel , F. Erhardt , N. B. Ezell , L. Fabbietti , U. Frankenfeld , J. J. Gaardhøje , C. Garabatos , P. Gasik , Á. Gera , P. Ghosh , S. K. Ghosh , P. Glässel , O. Grachov , A. Grein , T. Gunji , H. Hamagaki , G. Hamar , J. W. Harris , P. Hauer , J. Hehner , E. Hellbär , H. Helstrup , T. E. Hilden , B. Hohlweger , M. Ivanov , M. Jung , D. Just , E. Kangasaho , R. Keidel , B. Ketzer , S. A. Khan , S. Kirsch , T. Klemenz , S. Klewin , A. G. Knospe , M. Kowalski , L. Kumar , R. Lang , R. Langoy , L. Lautner , F. Liebske , J. Lien , C. Lippmann , H. M. Ljunggren , W. J. Llope , S. Mahmood , T. Mahmoud , R. Majka , P. Malzacher , A. Marín , C. Markert , S. Masciocchi , A. Mathis , A. Matyja , M. Meres , D. L. Mihaylov , D. Miskowiec , J. Mitra , T. Mittelstaedt , T. Morhardt , J. Mulligan , R. H. Munzer , K. Münning , M. G. Munhoz , S. Muhuri , H. Murakami , B. K. Nandi , H. Natal da Luz , C. Nattrass , T. K. Nayak , R. A. Negrao De Oliveira , M. Nicassio , B. S. Nielsen , L. Oláh , A. Oskarsson , J. Otwinowski , K. Oyama , G. Paić , R. N. Patra , V. Peskov , M. Pikna , L. Pinsky , M. Planinic , M. G. Poghosyan , N. Poljak , F. Pompei , S. K. Prasad , C. A. Pruneau , J. Putschke , S. Raha , J. Rak , J. Rasson , V. Ratza , K. F. Read , A. Rehman , R. Renfordt , T. Richert , K. Røed , D. Röhrich , T. Rudzki , R. Sahoo , S. Sahoo , P. K. Sahu , J. Saini , B. Schaefer , J. Schambach , S. Scheid , C. Schmidt , H. R. Schmidt , N. V Schmidt , H. Schulte , K. Schweda , I. Selyuzhenkov , N. Sharma , D. Silvermyr , R. N. Singaraju , B. Sitar , N. Smirnov , S. P. Sorensen , F. Sozzi , J. Stachel , E. Stenlund , P. Strmen , I. Szarka , G. Tambave , K. Terasaki , A. Timmins , K. Ullaland , A. Utrobicic , D. Varga , R. Varma , A. Velure , V. Vislavicius , S. Voloshin , B. Voss , D. Vranic , J. Wiechula , S. Winkler , J. Wikne , B. Windelband , C. Zhao

A large number of high-energy and heavy-ion experiments successfully used Time Projection Chamber (TPC) as central tracker and particle identification detector. However, the performance requirements on TPC for new high-rate particle…

Instrumentation and Detectors · Physics 2013-02-14 M. Poli Lener , M. Bazzi , G. Corradi , C. Curceanu , A. D'Uffizi , C. Paglia , A. Romero Vidal , E. Sbardella , A. Scordo , D. Tagnani , J. Zmeskal

The Gaseous Electron Multiplier-based Time Projection Chamber (GEM-TPC) in TWIN configuration for particle tracking has been consolidated after extensive investigations in different facilities to study its tracking performance. The most…

In this study, we developed a new proton detector system called CATCH, which was designed for a scattering experiment involving a $\Sigma$ hyperon and a proton (J-PARC E40). CATCH is a cylindrical detector system covering an inner target…

Instrumentation and Detectors · Physics 2022-03-14 Y. Akazawa , N. Chiga , N. Fujioka , S. H. Hayakawa , R. Honda , M. Ikeda , K. Matsuda , K. Miwa , Y. Nakada , T. Nanamura , S. Ozawa , T. Shiozaki , H. Tamura , H. Umetsu

Over the past several years the STAR experiment at RHIC has been contributing to our understanding of the proton structure. Through its instrumentation, STAR is well equipped to measure $W \rightarrow \nu + e$ in $\sqrt{s}$ = 500/510 GeV…

High Energy Physics - Experiment · Physics 2015-07-30 M. Posik

The next generation of detectors will detect gravitational waves from binary neutron stars at cosmological distances, for which around a thousand electromagnetic follow-ups may be observed per year. So far, most work devoted to the expected…

Cosmology and Nongalactic Astrophysics · Physics 2022-11-17 Viviane Alfradique , Miguel Quartin , Luca Amendola , Tiago Castro , Alexandre Toubiana

The STAR experiment at RHIC is carrying out a comprehensive high-energy spin physics program to understand the internal structure and dynamics of the proton in polarized proton-proton collisions at $\sqrt{s} = 200$ GeV and $\sqrt{s} =…

High Energy Physics - Experiment · Physics 2014-09-12 Xuan Li

A large Time Projection Chamber (TPC) is the main device for tracking and charged-particle identification in the ALICE experiment at the CERN LHC. After the second long shutdown in 2019-2020, the LHC will deliver Pb beams colliding at an…

Instrumentation and Detectors · Physics 2019-10-09 Piotr Gasik

Test beam measurements at the test beam facilities of DESY have been conducted to characterise the performance of the EUDET-type beam telescopes originally developed within the EUDET project. The beam telescopes are equipped with six sensor…

A prototype Secondary-electron Emission Monitor (SEM) was installed in the 8 GeV proton transport line for the MiniBooNE experiment at Fermilab. The SEM is a segmented grid made with 5 um Ti foils, intended for use in the 120 GeV NuMI beam…

Instrumentation and Detectors · Physics 2009-04-21 S. Kopp , D. Indurthy , Z. Pavlovich , M. Proga , R. Zwaska , S. Childress , R. Ford , C. Kendziora , T. Kobilarcik , C. Moore , G. Tassotto

The production of $W^{\pm}Z$ events in proton--proton collisions at a centre-of-mass energy of 13 TeV is measured with the ATLAS detector at the LHC. The collected data correspond to an integrated luminosity of 3.2 fb$^{-1}$. The $W^{\pm}Z$…

High Energy Physics - Experiment · Physics 2016-09-26 ATLAS Collaboration

Differential cross-section measurements are presented for the production of a $W$ boson in association with a photon. The analysis is performed using proton--proton collision data collected by the ATLAS experiment at $\sqrt{s}= 13$ TeV,…

High Energy Physics - Experiment · Physics 2026-03-25 ATLAS Collaboration

The next generation of collider experiments require tracking detectors with extreme performance capabilities in terms of spatial resolution (tens of $\mu \text{m}$), radiation hardness ($10^{17}~1~$MeV n$_{eq}/$cm$^2$) and timing resolution…

Instrumentation and Detectors · Physics 2023-01-05 Gian Matteo Cossu , Adriano Lai

The Gas Electron Multiplier (GEM) has become a widely used technology for high-rate particle physics experiments like COMPASS, LHCb and are being used as the readout system for the upcoming upgrade version of other experiments such as ALICE…

Instrumentation and Detectors · Physics 2021-05-26 Promita Roy , Purba Bhattacharya , Supratik Mukhopadhyay , Nayana Majumdar

The ALICE Collaboration is planning a major upgrade of its central barrel detectors to be able to cope with the increased LHC luminosity beyond 2020. For the TPC, this implies a replacement of the currently used gated MWPCs (Multi-Wire…

Instrumentation and Detectors · Physics 2019-08-13 Andreas Mathis

In view of a possible extension of the forward CMS muon detector system and future LHC luminosity upgrades, Micro-Pattern Gas Detectors (MPGDs) are an appealing technology. They can simultaneously provide precision tracking and fast trigger…

The STAR endcap electromagnetic calorimeter (EEMC) was designed to allow measurement of cross sections and spin observables in the forward direction, $1 < \eta < 2$ and with the full azimuth. Using the EEMC to measure double longitudinal…

High Energy Physics - Experiment · Physics 2019-08-14 S. Gliske , J. Drachenberg

For the International Large Detector (ILD), foreseen to be built at the International Linear Collider (ILC), a Time Projection Chamber (TPC) is intended to be used as the main tracking detector. The amplification will be provided by Micro…

Instrumentation and Detectors · Physics 2017-03-17 Paul Malek

A Time Projection Chamber (TPC) is an ideal device for the detection of charged particle tracks in a large volume covering a solid angle of almost $4\pi$. The high density of hits on a given particle track facilitates the task of pattern…

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
‹ Prev 1 8 9 10 Next ›