English
Related papers

Related papers: CMS-HF Calorimeter Upgrade for Run II

200 papers

The high flux of charged particles interacting with the CMS Forward Hadron Calorimeter PMT windows introduced a significant background for the trigger and offline data analysis. During Long Shutdown 1, all of the original PMTs were replaced…

Instrumentation and Detectors · Physics 2016-11-17 Emrah Tiras , Burak Bilki , Yasar Onel

The CMS Level-1 calorimeter trigger is being upgraded in two stages to maintain performance as the LHC increases pile-up and instantaneous luminosity in its second run. In the first stage, improved algorithms including event-by-event…

Hadronic Forward(HF) detector is one of the sub-detectors of the CMS. It plays an important role in the measurement of forward jets and missing energy. HF is situated on both sides of the CMS interaction point, at about $\pm$11 m, covers…

Instrumentation and Detectors · Physics 2020-09-23 Yalcin Guler

The physics program at the Fermilab Tevatron Collider will continue to explore the high energy frontier of particle physics until the commissioning of the LHC at CERN. The luminosity increase provided by the Main Injector will require…

Instrumentation and Detectors · Physics 2008-11-26 S. Kuhlmann , H. Frisch , M. Cordelli , J. Huston , R. Miller , S. Lami , R. Paoletti , N. Turini , M. Iori , D. Toback , T. Ukegawa

The CMS muon system operates gas-based detectors. Upgrades of the detectors and trigger components are needed to cope with increasingly challenging conditions of the HL-LHC. New irradiation tests are performed to ensure that the muon…

Instrumentation and Detectors · Physics 2018-09-07 Jian Wang

The electromagnetic ealorimeter (ECAL) of the CMS detector has played an important role in the physics program of the experiment, delivering outstanding performance throughout data taking. The High-Luminosity LHC will pose new challenges.…

Instrumentation and Detectors · Physics 2021-06-10 Stefano Argiro

The CMS experiment at the LHC has started data taking in Run 3 at a $\mathrm{pp}$ collision energy of $13.6~\mathrm{TeV}$. In preparation for Run 3, detector systems, such as Pixel Tracker, HCAL and CSC, have been upgraded due to…

High Energy Physics - Experiment · Physics 2023-09-07 Srećko Morović

The High Luminosity LHC (HL-LHC) phase is designed to increase by an order of magnitude the amount of data to be collected by the LHC experiments. The foreseen gradual increase of the instantaneous luminosity of up to more than twice its…

A new Beam Halo Monitor (BHM) detector system has been installed in the CMS cavern to measure the machine-induced background (MIB) from the LHC. This background originates from interactions of the LHC beam halo with the final set of…

Instrumentation and Detectors · Physics 2019-08-13 Kelly Stifter

Improving the coincidence time resolution (CTR) of time-of-flight positron emission tomography (TOF-PET) systems to achieve a higher signal-to-noise ratio (SNR) gain or even direct positron emission imaging (dPEI) is of paramount importance…

As the Tevatron luminosity increases sophisticated selections are required to be efficient in selecting rare events among a very huge background. To cope with this problem, CDF has pushed the offline calorimeter algorithm reconstruction…

Instrumentation and Detectors · Physics 2008-10-22 A. Canepa , M. Casarsa , T. Liu , G. Cortiana , G. Flanagan , H. Frisch , D. Krop , C. Pilcher , V. Rusu , V. Cavaliere , V. Greco , P. Giannetti , M. Piendibene , L. Sartori , M. Vidal

The HL-LHC phase is designed to increase by an order of magnitude the amount of data to be collected by the LHC experiments. To achieve this goal in a reasonable time scale the instantaneous luminosity would also increase by an order of…

The HL-LHC phase is designed to increase by an order of magnitude the amount of data to be collected by the LHC experiments. To achieve this goal in a reasonable time scale the instantaneous luminosity would also increase by an order of…

Instrumentation and Detectors · Physics 2016-09-21 F. Lagarde , M. Gouzevitch , I. Laktineh , V. Buridon , X. Chen , C. Combaret , A. Eynard , L. Germani , G. Grenier , H. Mathez , L. Mirabito , A. Petrukhin , A. Steen , W. Tromeuraa , Y. Wang , A. Gongab , N. Moreau , C. de la Taille , F. Dulucqac , A. Cimmino , S. Crucy , A. Fagot , M. Gul , A. A. O. Rios , M. Tytgat , N. Zaganidisb , S. Aly , Y. Assran , A. Radi , A. Sayedc , G. Singhd , M. Abbrescia , G. Iaselli , M. Maggi , G. Pugliese , P. Verwilligene , W. Van Doninck , S. Colafranceschi , A. Sharmag , L. Benussi , S. Bianco , D. Piccolo , F. Primaverah , V. Bhatnagar , R. Kumari , A. Mehta , J. Singhi , A. Ahmad , W. Ahmed , H. M. I. Asghar , I. M. Awan , R. Hoorani , S. Muhammad , H. Shahzad , M. A. Shah , S. W. Cho , S. Y. Choi , B. Hong , M. H. Kang , K. S. Lee , J. H. Lim , S. K. Parkk , M. S. Kiml , S. Carpinteyro Bernardino , I. Pedraza , C. Uribe Estradam , S. Carrillo Moreno , F. Vazquez Valencian , L. M. Panto , S. Buontempo , N. Cavallo , M. Esposito , F. Fabozzi , G. Lanza , I. Orso , L. Lista , S. Meola , M. Merola , P. Paolucci , F. Thyssen , A. Braghieri , A. Magnani , P. Montagna , C. Riccardi , P. Salvini , I. Vai , P. Vituloq , Y. Ban , S. J. Qianr , M. Choi , Y. Choi , J. Goh , D. Kimt , A. Aleksandrov , R. Hadjiiska , P. Iaydjiev , M. Rodozov , S. Stoykova , G. Sultanov , M. Vutovau , A. Dimitrov , L. Litov , B. Pavlov , P. Petkovv , I. Bagaturia , D. Lomidzew , C. Avila , A. Cabrera , J. C. Sanabria , I. Crottyy , J. Vaitkusz

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

During the upcoming High Luminosity phase of the Large Hadron Collider (HL-LHC), the integrated luminosity of the accelerator will increase to 3000 fb$^{-1}$. The expected experimental conditions in that period in terms of background rates,…

Instrumentation and Detectors · Physics 2022-01-19 A. Samalan , M. Tytgat , G. A. Alves , F. Marujo , F. Torres Da Silva De Araujo , E. M. DaCosta , D. De Jesus Damiao , H. Nogima , A. Santoro , S. Fonseca De Souza , A. Aleksandrov , R. Hadjiiska , P. Iaydjiev , M. Rodozov , M. Shopova , G. Soultanov , M. Bonchev , A. Dimitrov , L. Litov , B. Pavlov , P. Petkov , A. Petrov , S. J. Qian , C. Bernal , A. Cabrera , J. Fraga , A. Sarkar , S. Elsayed , Y. Assran , M. El Sawy , M. A. Mahmoud , Y. Mohammed , C. Combaret , M. Gouzevitch , G. Grenier , I. Laktineh , L. Mirabito , K. Shchablo , I. Bagaturia , D. Lomidze , I. Lomidze , V. Bhatnagar , R. Gupta , P. Kumari , J. Singh , V. Amoozegar , B. Boghrati , M. Ebraimi , R. Ghasemi , M. Mohammadi Najafabadi , E. Zareian , M. Abbrescia , R. Aly , W. Elmetenawee , N. DeFilippis , A. Gelmi , G. Iaselli , S. Leszki , F. Loddo , I. Margjeka , G. Pugliese , D. Ramos , M. Caponero , L. Benussi , S. Bianco , S. Colafranceschi , A. Russo , L. Passamonti , D. Piccolo , D. Pierluigi , G. Saviano , S. Buontempo , A. Di Crescenzo , F. Fienga , G. DeLellis , L. Lista , S. Meola , P. Paolucci , A. Braghieri , P. Salvini , P. Montagna , C. Riccardi , P. Vitulo , B. Francois , T. J. Kim , J. Park , S. Y. Choi , B. Hong , K. S. Lee , J. Goh , H. Lee , J. Eysermans , C. Uribe Estrada , I. Pedraza , H. Castilla-Valdez , A. Sanchez-Hernandez , C. A. Mondragon Herrera , D. A. Perez Navarro , G. A. AyalaSanchez , S. Carrillo , E. Vazquez , N. Zaganidis , A. Radi , A. Ahmad , I. Asghar , H. Hoorani , S. Muhammad , M. A. Shah , B. Mandelli , R. Guida , I. Crotty

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 High Luminosity LHC (HL-LHC) will integrate 10 times more luminosity than the LHC, posing significant challenges for radiation tolerance and event pileup on detectors, especially for forward calorimetry, and hallmarks the issue for…

Instrumentation and Detectors · Physics 2018-02-18 Arabella Martelli

We report on the design and performance of the electromagnetic calorimeter timing readout system (EMTiming) for the Collider Detector at Fermilab (CDF). The system will be used in searches for rare events with high energy photons to verify…

Instrumentation and Detectors · Physics 2008-11-26 M. Goncharov , T. Kamon , V. Khotilovich , V. Krutelyov , S. W. Lee , D. Toback , P. Wagner , H. Frisch , H. Sanders , M. Cordelli , F. Happacher , S. Miscetti , R. Wagner

The Muon Upgrade Phase II of the Compact Muon Solenoid (CMS) aims to guarantee the optimal conditions of the present system and extend the $\eta$ coverage to ensure a reliable system for the High Luminosity Large Hadron Collider (HL-LHC)…

Instrumentation and Detectors · Physics 2020-06-17 M. I. Pedraza-Morales

We are in the process of upgrading the VERITAS array of Cherenkov telescopes with new, high efficiency photomultipliers (PMT) that will considerably lower the energy threshold of the instrument and improve the overall sensitivity. The…

Instrumentation and Methods for Astrophysics · Physics 2019-08-13 A. Nepomuk Otte
‹ Prev 1 2 3 10 Next ›