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Related papers: The ALICE Muon IDentifier

200 papers

The ALICE experiment at the CERN Large Hadron Collider (LHC) is a multi-purpose particle detector, mainly focused on the study of quark-gluon plasma (QGP) in heavy-ion collisions. In the forward rapidity region, 2.5 $<$ y $<$ 4, ALICE is…

Nuclear Experiment · Physics 2024-11-04 Luca Quaglia , ALICE collaboration

A dedicated front-end electronics has been developed for the trigger chambers of the ALICE muon spectrometer which will work at the future LHC at CERN. These trigger chambers are based on RPCs (Resistive Plate Chambers) working in streamer…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. Rosnet , L. Royer , the Alice Collaboration

ALICE is the experiment dedicated to the study of the quark gluon plasma in heavy-ion collisions at the CERN LHC. Improvements of ALICE sub-detectors are envisaged for the upgrade plans of year 2017. The Muon Forward Tracker (MFT) is a…

High Energy Physics - Experiment · Physics 2012-01-04 Antonio Uras , Laure Marie Massacrier

The ALICE Collaboration will undertake a major upgrade of the detector apparatus during the second LHC Long Shutdown LS2 (2019-2020) in view of the Runs 3 and 4 (2021-2029). The objective of the upgrade is two-fold: i) an improvement of the…

Instrumentation and Detectors · Physics 2019-08-08 Gasik fo the ALICE Collaboration

The ALICE Collaboration is planning to construct a new detector (ALICE 3) aiming at exploiting the potential of the high-luminosity Large Hadron Collider (LHC). The new detector will allow ALICE to participate in LHC Run 5 scheduled from…

ALICE is the experiment dedicated to the study of the quark gluon plasma in heavy-ion collisions at the CERN LHC. Improvements of ALICE sub-detectors are envisaged for the upgrade plans of year 2017. The Muon Forward Tracker (MFT) is a…

High Energy Physics - Experiment · Physics 2019-08-14 Antonio Uras

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

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

During Phase-2 of the LHC, known as the High Luminosity LHC (HL-LHC), the accelerator will increase its instantaneous luminosity to 5 $\times$ 10$^{34}$ cm$^{-2}$ s$^{-1}$, delivering an integrated luminosity of 3000 fb$^{-1}$ over 10 years…

Instrumentation and Detectors · Physics 2020-07-24 Priyanka Kumari

ALICE (A Large Ion Collider Experiment) studies the Quark-Gluon Plasma (QGP): a deconfined state of matter obtained in ultra-relativistic heavy-ion collisions. One of the probes for QGP study are quarkonia and open heavy flavour, of which…

For Run 3 (from 2021), the LHC will undergo a significant increase in instantaneous luminosity to 1.5 times its current value which will lead to larger collected statistics and an enhanced sensitivity to new physics. The Phase-1 upgrade of…

Instrumentation and Detectors · Physics 2018-06-26 Shunichi Akatsuka

The ALICE Transition Radiation Detector contributes to the tracking, particle identification, and triggering capabilities of the experiment. It is composed of six layers of multi-wire proportional chambers, each of which is preceded by a…

Instrumentation and Detectors · Physics 2019-08-13 Jochen Klein

The Inner Tracking System (ITS) of the ALICE experiment will be upgraded during the second long LHC shutdown in $\mathrm{2019}-\mathrm{2020}$. The main goal of the ALICE ITS Upgrade is to enable high precision measurements of low - momentum…

Instrumentation and Detectors · Physics 2019-05-22 D. Andreou

The ALICE Collaboration completed the upgrade of the detector and is now commissioning for the beginning of the data taking during LHC Run 3. In parallel, R&D activities and simulation studies are being performed to define the future of the…

High Energy Physics - Experiment · Physics 2022-11-09 Domenico Colella , for the ALICE Collaboration

The LHC is expected to increase its center-of-mass energy from 13 TeV to 14 TeV for Run 3 scheduled from 2022 to 2024. After Run 3, upgrades for the High-Luminosity-LHC (HL-LHC) programme are planned and the operation will start in 2027,…

Instrumentation and Detectors · Physics 2021-09-01 Yuya Mino

ALICE (A Large Ion Collider Experiment) experiment at CERN LHC is designed to study the properties of the Quark-Gluon Plasma (QGP) in heavy-ion collisions. In 2019-2020 the upgrade of CERN LHC will increase the luminosity and the collision…

Instrumentation and Detectors · Physics 2019-05-01 A. I. Maevskaya

The Level-1 Muon Barrel Trigger of the ATLAS Experiment at LHC makes use of Resistive Plate Chamber (RPC) detectors. The on-detector trigger electronics modules are able to identify muons with predefined transverse momentum values (pT) by…

Instrumentation and Detectors · Physics 2018-06-27 V. Izzo , A. Aloisio , R. Giordano , S. Perrella , R. Vari

A new type of Time Projection Chamber (TPC) has been proposed for the upgrade of the ALICE (A Large Ion Collider Experiment at CERN) so as to cater to the high luminosity environment expected at the Large Hadron Collider (LHC) facility in…

Instrumentation and Detectors · Physics 2015-11-17 Saikat Biswas

ALICE, one of the experiments at the Large Hadron Collider (CERN), is undergoing ambitious upgrades during the ongoing second long shutdown (LS2). The main goal of this project is to access rare events and previously inaccessible physics…

Instrumentation and Detectors · Physics 2020-04-23 Adam Laszlo Gera

ALICE (A Large Ion Collider Experiment) is the heavy-ion detector designed to study the strongly interacting state of matter realized in relativistic heavy-ion collisions at the CERN Large Hadron Collider (LHC). A major upgrade of the…

Instrumentation and Detectors · Physics 2019-08-14 Pascal Boeschoten , Filippo Costa