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The preliminary results of an aging test performed at the CERN Gamma Irradiation Facility on a single--gap RPC prototype developed for the LHCb Muon System are presented. The results are based on an accumulated charge density of 0.42…

We present recent results of an extensive aging test, performed at the CERN Gamma Irradiation Facility on two single--gap RPC prototypes, developed for the LHCb Muon System. With a method based on a model describing the behaviour of an RPC…

In the High Luminosity Large Hadron Collider (HL-LHC) program, during the next years, the instantaneous luminosity will increase up to 5 $\times$ 10$^{34}$ cm$^{-2}$ s$^{-1}$ which means a factor five higher than the nominal LHC. In that…

Instrumentation and Detectors · Physics 2021-11-30 R. Aly

The CMS Resistive Plate Chamber (RPC) system has been certified for 10 years of LHC operation. In the next years, during the High luminosity LHC (HL-LHC) phase, the LHC instantaneous luminosity will increase to a factor five more than the…

Instrumentation and Detectors · Physics 2022-08-31 R. Aly

The muon spectrometer of the CMS (Compact Muon Solenoid) experiment at the Large Hadron Collider (LHC) is equipped with a redundant system made of Resistive Plate Chambers and Drift Tube in barrel and RPC and Cathode Strip Chamber in endcap…

Instrumentation and Detectors · Physics 2015-06-22 G. Pugliese

The muon spectrometer of the CMS (Compact Muon Solenoid) experiment at the Large Hadron Collider (LHC) is equipped with a redundant system made of Resistive Plate Chambers (RPCs) and Drift Tube (DT) chambers in the barrel, RPC and Cathode…

Instrumentation and Detectors · Physics 2017-06-22 M. I. Pedraza-Morales , M. A. Shaha , M. Shopova

The muon detector of LHCb, which comprises 1368 multi-wire-proportional-chambers (MWPC) for a total area of 435 m2, is the largest instrument of its kind exposed to such a high-radiation environment. In nine years of operation, from 2010…

An ageing test of three ATLAS production RPC stations is in course at X5-GIF, the CERN irradiation facility. The chamber efficiencies are monitored using cosmic rays triggered by a scintillator hodoscope. Higher statistics measurements are…

With the HL-LHC upgrade of the LHC machine, an increase of the instantaneous luminosity by a factor of five is expected and the current detection systems need to be validated for such working conditions to ensure stable data taking. At the…

Instrumentation and Detectors · Physics 2023-05-17 K. Mota Amarilo , A. Samalan , M. Tytgat , M. El Sawy , G. A. Alves , F. Marujo , E. A. Coelho , E. M. Da Costa , H. Nogima , A. Santoro , S. Fonseca De Souza , D. De Jesus Damiao , M. Thiel , M. Barroso Ferreira Filho , A. Aleksandrov , R. Hadjiiska , P. Iaydjiev , M. Rodozov , M. Shopova , G. Soultanov , A. Dimitrov , L. Litov , B. Pavlov , P. Petkov , A. Petrov , E. Shumka , S. J. Qian , H. Kou , Z. -A. Liu , J. Zhao , J. Song , Q. Hou , W. Diao , P. Cao , C. Avila , D. Barbosa , A. Cabrera , A. Florez , J. Fraga , J. Reyes , Y. Assran , M. A. Mahmoud , Y. Mohammed , I. Crotty , I. Laktineh , G. Grenier , M. Gouzevitch , L. Mirabito , K. Shchablo , I. Bagaturia , I. Lomidze , Z. Tsamalaidze , V. Amoozegar , B. Boghrati , M. Ebraimi , M. Mohammadi Najafabadi , E. Zareian , M. Abbrescia , G. Iaselli , G. Pugliese , F. Loddo , N. De Filippis , R. Aly , D. Ramos , W. Elmetenawee , S. Leszki , I. Margjeka , D. Paesani , L. Benussi , S. Bianco , D. Piccolo , S. Meola , S. Buontempo , F. Carnevali , L. Lista , P. Paolucci , F. Fienga , A. Braghieri , P. Salvini , P. Montagna , C. Riccardi , P. Vitulo , E. Asilar , J. Choi , T. J. Kim , S. Y. Choi , B. Hong , K. S. Lee , H. Y. Oh , J. Goh , I. Yu , C. Uribe Estrada , I. Pedraza , H. Castilla-Valdez , A. Sanchez-Hernandez , R. L. Fernandez , M. Ramirez-Garcia , E. Vazquez , M. A. Shah , N. Zaganidis , A. Radi , H. Hoorani , S. Muhammad , A. Ahmad , I. Asghar , W. A. Khan , J. Eysermans , F. Torres Da Silva De Araujo

The Muon Chamber (MuCh) is a sub-system of the Compressed Baryonic Matter (CBM) experiment for the detection of low-mass-vector mesons produced in high energy heavy-ion collisions at beam energies ranging from 2 AGeV to 11 AGeV and decaying…

Instrumentation and Detectors · Physics 2022-01-04 Mitali Mondal , Tanay Dey , Subhasis Chattopadhyay , Jogender Saini , Zubayer Ahammed

Experimental conditions at the HERA-B experiment impose very strong requirements for gaseous detectors. The charged particle fluxes through the HERA-B tracking system, varying with the radial distance $R$ from the beam line, are about $2…

High Energy Physics - Experiment · Physics 2007-05-23 M. Danilov , Yu. Gilitsky , T. Kvaratschellia , L. Laptin , I. Tichomirov , M. Titov , Yu. Zaitsev

The characteristics of triple GEM detectors have been studied systematically by using cosmic ray muons. The minimum ionizing particle (MIP) spectra has been taken for different GEM voltage setting. Efficiency of GEM detector has been…

Instrumentation and Detectors · Physics 2015-06-17 S. Biswas , D. J. Schmidt , A. Abuhoza , U. Frankenfeld , C. Garabatos , J. Hehner , V. Kleipa , T. Morhardt , C. J. Schmidt , H. R. Schmidt , J. Wiechula

The CMS experiment, located at the CERN Large Hadron Collider, has a redundant muon system composed by three different detector technologies: Cathode Strip Chambers (in the forward regions), Drift Tubes (in the central region) and Resistive…

The CMS drift tubes (DT) muon detector, built for withstanding the LHC expected integrated and instantaneous luminosities, will be used also in the High Luminosity LHC (HL-LHC) at a 5 times larger instantaneous luminosity and, consequently,…

Instrumentation and Detectors · Physics 2019-12-16 G. Abbiendi , J. Alcaraz Maestre , A. Álvarez Fernández , B. Álvarez González , N. Amapane , I. Bachiller , J. M. Barcala , L. Barcellan , C. Battilana , M. Bellato , G. Bencze , M. Benettoni , N. Beni , A. Benvenuti , L. C. Blanco Ramos , A. Boletti , A. Bragagnolo , J. A. Brochero Cifuentes , V. Cafaro , A. Calderon , E. Calvo , A. Cappati , R. Carlin , C. A. Carrillo Montoya , F. R. Cavallo , J. M. Cela Ruiz , M. Cepeda , M. Cerrada , B. Chazin Quero , P. Checchia , L. Ciano , N. Colino , D. Corti , G. Cotto , J. Cuevas , M. Cuffiani , G. M. Dallavalle , D. Dattola , B. De La Cruz , P. DeRemigis , C. Erice Cid , F. Fabbri , A. Fanfani , D. Fasanella , C. F. Bedoya , J. F. de Trocóniz , P. Fernandez Manteca , J. Fernández Menéndez , J. P. Fernández Ramos , S. Folgueras , M. C. Fouz , D. Francia Ferrero , J. García Romero , F. Gasparini , U. Gasparini , S. Ghosh , V. Giordano , F. Gomez Casademunt , F. Gonella , I. González Caballero , J. R. González Fernández , O. González López , S. Goy López , A. Gozzelino , A. Griggio , G. Grosso , C. Guandalini , L. Guiducci , M. Gulmini , T. Hebbeker , C. Heidemann , J. M. Hernández , K. Hoepfner , F. Iemmi , R. Isocrate , M. I. Josa , B. Kiani , S. Lacaprara , S. Lo Meo , S. Marcellini , M. Margoni , J. Marín , C. Mariotti , I. Martín Martín , J. J. Martínez Morales , C. Martínez Rivero , S. Maselli , G. Masetti , A. T. Meneguzzo , M. Merschmeyer , G. Mocellin , L. Modenese , A. Molinero , J. Molnar , F. Montecassiano , D. Moran , J. J. Navarrete , F. Navarria , Á. Navarro Tobar , J. C. Oller , M. Passaseo , J. Pazzini , M. Pegoraro , J. Puerta Pelayo , M. Pelliccioni , B. Philipps , J. Piedra Gomez , G. L. Pinna Angioni , N. Pozzobon , M. Presilla , C. Prieels , F. Primavera , J. C. Puras Sánchez , I. Redondo , D. D. Redondo Ferrero , H. Reithler , T. Rodrigo , V. Rodríguez Bouza , J. Roemer , P. Ronchese , R. Rossin , F. Rotondo , T. Rovelli , S. Sánchez Cruz , S. Sánchez Navas , J. Sastre , L. Scodellaro , F. Simonetto , M. S. Soares , A. Staiano , Z. Szillasi , D. F. Teyssier , N. Toniolo , E. Torassa , D. Trocino , B. Ujvari , S. Ventura , R. Vilar Cortabitarte , J. Vizan Garcia , M. Zanetti , F. P. Zantis , G. Zilizi , P. Zotto

With the constant increase of accelerator luminosity, the rate requirements of the MRPC detectors become important. In the same time, aging problem of the detector has to be studied meticulously. An online aging test system is set up in our…

Instrumentation and Detectors · Physics 2016-08-03 Jie Wang , Yi Wang , S. Q. Feng , Bo Xie , Pengfei Lv , Fuyue Wang , Baohong Guo , Dong Han , Yuanjing Li

Experimental conditions at the HERA-B experiment impose very strong requirements for gaseous detectors. The charged particle fluxes through the HERA-B tracking system, varying with the radial distance R from the beam line, are about $2…

High Energy Physics - Experiment · Physics 2007-05-23 M. Danilov , Yu. Gilitsky , T. Kvaratschellia , L. Laptin , I. Tichomirov , M. Titov , Yu. Zaitsev

In the framework of the High Luminosity LHC upgrade program, the CMS muon group built several different RPC prototypes that are now under test at the new CERN Gamma Irradiation Facility (GIF++). A dedicated Detector Control System has been…

Instrumentation and Detectors · Physics 2019-08-13 Muhammad Gul , Genoveva Gonzalez

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
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