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A full replacement of the existing muon trigger system in the CMS (Compact Muon Solenoid) detector is planned for operating at the maximum instantaneous luminosities of about $5-7.5\times10^{34}$ cm$^{-2}$ s$^{-1}$ expected in HL-LHC (High…

Instrumentation and Detectors · Physics 2019-11-01 Silvia Goy López

The Large Hadron Collider (LHC) started the Run 3 operation in 2022, and the peak instantaneous luminosity in Run 3 may reach 3 x 10^34 cm-2s-1. The ATLAS Monitored Drift Tube (MDT) chambers are the main component of the precision tracking…

Instrumentation and Detectors · Physics 2026-02-04 Jiajin Ge , Bing Li , Markus Fras , Junjie Zhu , Bing Zhou , Tiesheng Dai

The muon system of the CMS experiment is expected to upgrade all of its subdetectors for the Phase-2 of the Large Hadron Collider (LHC) that will begin in 2029. The upgrade plans for drift tubes (DTs), cathode strip chambers (CSCs) and…

Instrumentation and Detectors · Physics 2023-12-19 Antonello Pellecchia

The Monitored Drift Tube (MDT) chambers for the muon spectrometer of the AT- LAS detector at the Large Hadron Collider (LHC) consist of 3-4 layers of pressurized drift tubes on either side of a space frame carrying an optical monitoring…

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

Small-diameter Drift Tube (sMDT) detectors with 15 mm tube diameter have proven to be excellent candidates for precision muon tracking detectors in experiments at future hadron colliders like HL-LHC and FCC-hh where unprecedentedly high…

Instrumentation and Detectors · Physics 2021-12-13 G. H. Eberwein , O. Kortner , H. Kroha , E. Voevodina

ATLAS muon detector upgrades aim for increased acceptance for muon triggering and precision tracking and for improved rate capability of the muon chambers in the high-background regions of the detector with increasing LHC luminosity. The…

Instrumentation and Detectors · Physics 2017-03-08 Hubert Kroha , Oliver Kortner , Korbinian Schmidt-Sommerfeld , Eric Takasugi

Pressurized drift-tube chambers are efficient detectors for high-precision tracking over large areas. The Monitored Drift-Tube (MDT) chambers of the muon spectrometer of the ATLAS detector at the Large Hadron Collider (LHC) reach a spatial…

Instrumentation and Detectors · Physics 2016-10-04 B. Bittner , J. Dubbert , S. Horvat , O. Kortner , H. Kroha , F. Legger , R. Richter , S. Adomeit , O. Biebel , A. Engl , R. Hertenberger , F. Rauscher , A. Zibell

The Monitored Drift Tube (MDT) chambers for the muon spectrometer of the ATLAS detector at the Large Hadron Collider (LHC) consist of 3-4 layers of pressurised drift tubes on either side of a space frame carrying an optical deformation…

The CMS muon system includes in both the barrel and endcap region Resistive Plate Chambers (RPC). They mainly serve as trigger detectors and also improve the reconstruction of muon parameters. Over the years, the instantaneous luminosity of…

At the High Luminosity LHC (HL-LHC), the CMS experiment will need to operate at up to 200 interactions per 25 ns beam crossing time and with up to 4000 fb-1 of integrated luminosity. To achieve the physics goals the experiment needs to…

Instrumentation and Detectors · Physics 2022-12-21 A. La Rosa , I. Ahmed , J. Almeida , G. Blanchot , S. Cooperstein , I. Dominguez , A. Honma , M. Kovacs , A. Zografos

In the ATLAS Muon Spectrometer, Monitored Drift Tube (MDT) chambers and sMDT chambers with half of the tube diameter of the MDTs are used for precision muon track reconstruction. The sMDT chambers are designed for operation at high counting…

Experiments like ATLAS at the HL-LHC or detectors at future hadron colliders need muon detectors with excellent momentum resolution up to the TeV scale both at the trigger and offline reconstruction levels. This requires muon tracking…

New front-end electronics including ASICs and FPGA boards are under development for the ATLAS Monitored Drift Tube (MDT) detector to handle the large data rates and harsh environment expected at high-luminosity LHC runs. A mobile Data…

Instrumentation and Detectors · Physics 2022-11-23 Yuxiang Guo , Xueye Hu , Thomas Schwarz , Bing Zhou , Junjie Zhu

Small-diameter muon drift tube (sMDT) chambers with 15 mm tube diameter are a cost-effective technology for high-precision muon tracking over large areas at high background rates as expected at future high-energy hadron colliders including…

Instrumentation and Detectors · Physics 2017-03-08 Philipp Gadow , Oliver Kortner , Hubert Kroha , Robert Richter

The High-Luminosity LHC (HL-LHC) will usher in a new era in high-energy physics. The HL-LHC experimental conditions entail an instantaneous luminosity of up to $7.5 \times 10^{34}$ cm$^{-2}$ s$^{-1}$ and up to 200 simultaneous collisions…

High Energy Physics - Experiment · Physics 2022-11-17 Thiago R. F. P. Tomei

Highly selective triggers are essential for the physics programme of the ATLAS experiment at HL-LHC where the instantaneous luminosity will be about an order of magnitude larger than the LHC instantaneous luminosity in Run 1. The first…

Instrumentation and Detectors · Physics 2016-10-04 H. Kroha , S. Nowak

The performance of pressurized drift-tube detectors at very high background rates has been studied at the Gamma Irradiation Facility (GIF) at CERN and in an intense 20 MeV proton beam at the Munich Van-der-Graaf tandem accelerator for…

The Compact Muon Solenoid (CMS) experiment prepares its Phase-2 upgrade for the high-luminosity era of the LHC operation (HL-LHC). Due to the increase of occupancy, trigger latency and rates, the full electronics of the CMS Drift Tube (DT)…

High Energy Physics - Experiment · Physics 2023-02-06 G. Abbiendi , J. Alcaraz Maestre , A. Álvarez Fernández , B. Álvarez González , N. Amapane , I. Bachiller , L. Barcellan , C. Baldanza , C. Battilana , M. Bellato , G. Bencze , M. Benettoni , N. Beni , A. Benvenuti , A. Bergnoli , L. C. Blanco Ramos , L. Borgonovi , A. Bragagnolo , V. Cafaro , A. Calderon , E. Calvo , R. Carlin , C. A. Carrillo Montoya , F. R. Cavallo , J. M. Cela Ruiz , M. Cepeda , M. Cerrada , P. Checchia , L. Ciano , N. Colino , D. Corti , G. Cotto , A. Crupano , S. Cuadrado Calzada , J. Cuevas , M. Cuffiani , G. M. Dallavalle , D. Dattola , B. De La Cruz , C. I. de Lara Rodríguez , P. De Remigis , C. Erice Cid , D. Eliseev , F. Fabbri , A. Fanfani , D. Fasanella , C. F. Bedoya , J. F. de Trocóniz , D. Fernández del Val , J. Fernández Menéndez , J. P. Fernández Ramos , S. Folgueras , M. C. Fouz , D. Francia Ferrero , J. García Romero , F. Gasparini , U. Gasparini , V. Giordano , 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 , K. Hoepfner , R. Isocrate , M. I. Josa , B. Kiani , J. León Holgado , S. Lo Meo , E. Lusiani , L. Lunerti , S. Marcellini , M. Margoni , C. Mariotti , I. Martín Martín , J. J. Martínez Morales , S. Maselli , G. Masetti , A. T. Meneguzzo , M. Merschmeyer , M. Migliorini , L. Modenese , J. Molnar , F. Montecassiano , J. Mora Martínez , D. Moran , S. Mukherjee , J. J. Navarrete , F. Navarria , A. Navarro Tobar , F. Nowotny , E. Palencia Cortezón , M. Passaseo , J. Pazzini , M. Pelliccioni , A. Perrotta , B. Philipps , J. Piedra Gomez , F. Primavera , J. Puerta Pelayo , J. C. Puras Sánchez , C. Ramón Álvarez , I. Redondo , D. D. Redondo Ferrero , H. Reithler , R. Reyes-Almanza , V. Rodríguez Bouza , P. Ronchese , A. M. Rossi , R. Rossin , F. Rotondo , T. Rovelli , S. Sánchez Cruz , S. Sánchez Navas , J. Sastre , A. Sharma , F. Simonetto , A. Soto Rodríguez , A. Staiano , Z. Szillasi , D. F. Teyssier , N. Toniolo , G. Torromeo , A. Trapote , N. Trevisani , A. Triossi , D. Trocino , B. Ujvari , G. Umoret , L. Urda Gómez , B. Uwe , S. Ventura , C. Vico Villalba , S. Wiedenbeck , M. Zanetti , F. P. Zantis , G. Zilizi , P. Zotto , A. Zucchetta
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