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The ALICE experiment features multiple particle identification systems. The measurement of the identified charged hadron $p_{t}$ spectra in proton-proton collisions at $\sqrt{s}=900$ GeV will be discussed. In the central rapidity region…

High Energy Physics - Experiment · Physics 2019-08-14 L. Milano

Silicon microstrip detectors are widely used in experiments for space astronomy. Before the detector is assembled, extensive characterization of the silicon microstrip sensors is indispensable and challenging. This work electrically…

Instrumentation and Detectors · Physics 2021-03-29 Jia-Ju Wei , Jian-Hua Guo , Yi-Ming Hu

The present document discusses plans for a compact, next-generation multi-purpose detector at the LHC as a follow-up to the present ALICE experiment. The aim is to build a nearly massless barrel detector consisting of truly cylindrical…

Instrumentation and Detectors · Physics 2019-05-03 D. Adamová , G. Aglieri Rinella , M. Agnello , Z. Ahammed , D. Aleksandrov , A. Alici , A. Alkin , T. Alt , I. Altsybeev , D. Andreou , A. Andronic , F. Antinori , P. Antonioli , H. Appelshäuser , R. Arnaldi , I. C. Arsene , M. Arslandok , R. Averbeck , M. D. Azmi , X. Bai , R. Bailhache , R. Bala , L. Barioglio , G. G. Barnaföldi , L. S. Barnby , P. Bartalini , K. Barth , S. Basu , F. Becattini , C. Bedda , I. Belikov , F. Bellini , R. Bellwied , S. Beole , L. Bergmann , R. A. Bertens , M. Besoiu , L. Betev , A. Bhatti , A. Bianchi , L. Bianchi , J. Bielčík , J. Bielčíková , A. Bilandzic , S. Biswas , R. Biswas , D. Blau , F. Bock , M. Bombara , M. Borri , P. Braun-Munzinger , M. Bregant , G. E. Bruno , M. D. Buckland , H. Buesching , S. Bufalino , P. Buncic , J. B. Butt , A. Caliva , P. Camerini , F. Carnesecchi , J. Castillo Castellanos , F. Catalano , S. Chapeland , M. Chartier , C. Cheshkov , B. Cheynis , V. Chibante Barroso , D. D. Chinellato , P. Chochula , T. Chujo , C. Cicalo , F. Colamaria , D. Colella , M. Concas , Z. Conesa del Valle , G. Contin , J. G. Contreras , F. Costa , B. Dönigus , T. Dahms , A. Dainese , J. Dainton , A. Danu , S. Das , D. Das , S. Dash , A. Dash , G. David , A. De Caro , G. de Cataldo , A. De Falco , N. De Marco , S. De Pasquale , S. Deb , D. Di Bari , A. Di Mauro , T. Dietel , R. Divià , U. Dmitrieva , A. Dobrin , A. K. Dubey , A. Dubla , D. Elia , B. Erazmus , A. Erokhin , G. Eulisse , D. Evans , L. Fabbietti , M. Faggin , P. Fecchio , A. Feliciello , G. Feofilov , A. Fernández Téllez , A. Festanti , S. Floerchinger , P. Foka , S. Fokin , A. Franco , C. Furget , A. Furs , J. Gaardhøje , M. Gagliardi , P. Ganoti , C. Garabatos , E. Garcia-Solis , C. Gargiulo , P. Gasik , M. B. Gay Ducati , M. Germain , P. Ghosh , P. Giubellino , P. Giubilato , P. Glässel , V. Gonzalez , O. Grachov , A. Grigoryan , S. Grigoryan , F. Grosa , J. F. Grosse-Oetringhaus , R. Guernane , T. Gunji , R. Gupta , A. Gupta , M. K. Habib , H. Hamagaki , J. W. Harris , D. Hatzifotiadou , S. T. Heckel , E. Hellbär , H. Helstrup , T. Herman , H. Hillemanns , C. Hills , B. Hippolyte , S. Hornung , P. Hristov , J. P. Iddon , S. Igolkin , G. Innocenti , M. Ippolitov , M. Ivanov , A. Jacholkowski , M. Jung , A. Jusko , M. K. Köhler , S. Kabana , A. Kalweit , A. Karasu Uysal , T. Karavicheva , U. Kebschull , R. Keidel , M. Keil , B. Ketzer , S. A. Khan , A. Khanzadeev , Y. Kharlov , A. Khuntia , B. Kim , J. Kim , M. Kim , J. Klein , C. Klein , C. Klein-Bösing , S. Klewin , A. Kluge , M. L. Knichel , C. Kobdaj , M. Kofarago , P. J. Konopka , V. Kovalenko , I. Králik , M. Krüger , L. Kreis , M. Krivda , F. Krizek , M. Kroesen , E. Kryshen , V. Kučera , C. Kuhn , L. Kumar , S. Kundu , S. Kushpil , M. J. Kweon , M. Kwon , Y. Kwon , P. Lévai , S. L. La Pointe , E. Laudi , T. Lazareva , R. Lea , L. Leardini , S. Lee , R. C. Lemmon , R. Lietava , B. Lim , V. Lindenstruth , A. Lindner , C. Lippmann , J. Liu , J. Lopez Lopez , C. Lourenco , G. Luparello , S. M. Mahmood , A. Maire , V. Manzari , Y. Mao , A. Marín , M. Marchisone , G. V. Margagliotti , M. Marquard , P. Martinengo , S. Masciocchi , M. Masera , E. Masson , A. Mastroserio , A. M. Mathis , A. Matyja , M. Mazzilli , M. A. Mazzoni , L. Micheletti , A. N. Mishra , D. Miskowiec , B. Mohanty , M. Mohisin Khan , A. Morsch , T. Mrnjavac , V. Muccifora , D. Mühlheim , S. Muhuri , J. D. Mulligan , M. G. Munhoz , R. H. Munzer , H. Murakami , L. Musa , B. Naik , B. K. Nandi , R. Nania , T. K. Nayak , D. Nesterov , G. Nicosia , S. Nikolaev , V. Nikulin , F. Noferini , J. Norman , A. Nyanin , V. Okorokov , C. Oppedisano , J. Otwinowski , K. Oyama , M. Płoskoń , Y. Pachmayer , A. K. Pandey , C. Pastore , J. Pawlowski , H. Pei , T. Peitzmann , D. Peresunko , M. Petrovici , R. P. Pezzi , S. Piano , E. Prakasa , S. K. Prasad , R. Preghenella , F. Prino , C. A. Pruneau , I. Pshenichnov , M. Puccio , J. Pucek , E. Quercigh , D. Röhrich , L. Ramello , F. Rami , S. Raniwala , R. Raniwala , R. Rath , I. Ravasenga , A. Redelbach , K. Redlich , F. Reidt , K. Reygers , V. Riabov , P. Riedler , W. Riegler , D. Rischke , C. Ristea , S. P. Rode , M. Rodríguez Cahuantzi , D. Rohr , A. Rossi , R. Rui , A. Rustamov , A. Rybicki , K. Šafařík , R. Sadikin , S. Sadovsky , R. Sahoo , P. Sahoo , P. K. Sahu , J. Saini , V. Samsonov , P. Sarma , H. S. Scheid , R. Schicker , A. Schmah , M. O. Schmidt , C. Schmidt , Y. Schutz , K. Schweda , E. Scomparin , J. E. Seger , S. Senyukov , A. Seryakov , R. Shahoyan , N. Sharma , S. Siddhanta , T. Siemiarczuk , R. Singh , M. Sitta , H. Soltveit , M. Spyropoulou-Stassinaki , J. Stachel , T. Sugitate , S. Sumowidagdo , X. Sun , J. Takahashi , C. Terrevoli , A. Toia , N. Topilskaya , S. Tripathy , S. Trogolo , V. Trubnikov , W. H. Trzaska , B. A. Trzeciak , T. S. Tveter , A. Uras , G. L. Usai , G. Valentino , L. V. R. van Doremalen , M. van Leeuwen , P. Vande Vyvre , M. Vasileiou , V. Vechernin , L. Vermunt , O. Villalobos Baillie , T. Virgili , A. Vodopyanov , S. A. Voloshin , G. Volpe , B. von Haller , I. Vorobyev , Y. Wang , M. Weber , A. Wegrzynek , D. F. Weiser , S. C. Wenzel , J. P. Wessels , J. Wiechula , U. Wiedemann , J. Wilkinson , B. Windelband , M. Winn , N. Xu , K. Yamakawa , Z. Yin , I. -K. Yoo , J. H. Yoon , A. Yuncu , V. Zaccolo , C. Zampolli , A. Zarochentsev , B. Zhang , X. Zhang , C. Zhao , V. Zherebchevskii , D. Zhou , Y. Zhou , Y. Zhou , G. Zinovjev

The LHCb detector has undergone a major upgrade for LHC Run 3. This Upgrade I detector facilitates operation at higher luminosity and utilises full-detector information at the LHC collision rate, critically including the use of vertex…

In the planned or considered upgrades of LHCb, ALICE and Belle II experiments, the Ring imaging Cherenkov (RICH) detectors will have to be improved in order to function at increased beam interaction density. The photodetectors used in…

The high-luminosity upgrade of the CERN LHC requires the replacement of the CMS tracking detector to cope with the increased radiation fluence while maintaining its excellent performance. An extensive R\&D program, aiming at using 3D pixel…

Instrumentation and Detectors · Physics 2025-10-16 The Tracker Group of the CMS Collaboration

The planned upgrade of the LHC accelerator at CERN, namely the high luminosity (HL) phase of the LHC (HL-LHC foreseen for 2023), will result in a more intense radiation environment than the present tracking system was designed for. The…

Instrumentation and Detectors · Physics 2015-12-09 Timo Peltola

A detailed study of pseudorapidity densities and multiplicity distributions of primary charged particles produced in proton-proton collisions, at $\sqrt{s} =$ 0.9, 2.36, 2.76, 7 and 8 TeV, in the pseudorapidity range $|\eta|<2$, was carried…

Nuclear Experiment · Physics 2017-04-04 ALICE Collaboration

sPHENIX is the first new collider detector experiment dedicated to heavy-ion physics since the LHC began collecting data. Successfully commissioned in 2023-2024, one of its standout features is a streaming-capable tracking system that…

Nuclear Experiment · Physics 2025-11-04 Xudong Yu

The relativistic heavy ion collider (RHIC) offers many opportunities to study diffraction in pp, pA and AA collisions. Because both proton beams can be polarized, RHIC offers the unique possibility of studying polarization effects in…

High Energy Physics - Experiment · Physics 2008-11-26 A. Bravar , W. Guryn , S. R. Klein , D. Milstead , B. Surrow

Following the Phase-II upgrade during Long Shutdown (LS3), the LHC aims to reach a peak instantaneous luminosity of $7.5\times 10^{34}$cm$^{-2}$s$^{-1}$, which corresponds to an average of around 200 inelastic proton-proton collisions per…

The charged particle multiplicity distribution is one of the first measurements that ALICE will be able to perform. The knowledge of this basic property at a new energy is needed to configure Monte Carlo generators correctly with the aim of…

High Energy Physics - Experiment · Physics 2011-05-05 J. F. Grosse-Oetringhaus

Reliable hardware connectivity is vital in heterogeneous integrated systems. For example, in digital microfluidics lab-on-a-chip systems, there are hundreds of physical connections required between a micro-electro-mechanical fabricated…

Systems and Control · Electrical Eng. & Systems 2020-04-15 Chunjie Zhang , Yang Su , Siyi Hu , Kai Jin , Yuhan Jie , Wenshi Li , Arokia Nathan , Hanbin Ma

LHCb is the dedicated heavy flavour experiment at the Large Hadron Collider at CERN. The partially assembled silicon vertex locator (VELO) of the LHCb experiment has been tested in a beam test. The data from this beam test have been used to…

Instrumentation and Detectors · Physics 2008-11-26 M. Gersabeck , S. Viret , C. Parkes

Results are presented from the ATLAS collaboration from the 2010 LHC heavy ion run, during which nearly 10 inverse microbarns of luminosity were delivered. Soft physics results include charged particle multiplicities and collective flow.…

Nuclear Experiment · Physics 2015-05-28 Peter Steinberg , ATLAS Collaboration

In the paper, we discuss the development of the multi-gap resistive plate chamber Time-of-Flight (TOF) technology and the production of the STAR TOF detector in China at the beginning of the 21st century. Then we review recent experimental…

The ePIC detector is being designed as a general-purpose detector to deliver the full physics program of the Electron-Ion Collider (EIC) in BNL USA. Particle Identification (PID) plays a crucial role in the EIC physics program. Over a wide…

Instrumentation and Detectors · Physics 2025-01-07 Chandradoy Chatterjee

The exploration of the QCD phase diagram has been one of the main drivers of contemporary nuclear physics. The Relativistic Heavy Ion Collider (RHIC) at BNL is uniquely suited for this task through its Beam Energy Scan (BES) program which…

Nuclear Experiment · Physics 2018-10-12 David Tlusty

Two samples of silicon pad sensors and two samples of GaAs sensors are studied in an electron beam with 5 GeV energy from the DESY-II test-beam facility. The sizes of the silicon and GaAs sensors are about 9$\times$9 cm$^2$ and 5$\times$8…

The Electron-ion collider in China (EicC) is a proposed future electron-ion collider designed to achieve a high luminosity, with a center-of-mass energy ranging from 15 to 20 GeV. Excellent particle identification (PID) with extensive…

Instrumentation and Detectors · Physics 2026-05-25 Xin Li , Yuxiang Zhao , Yutie Liang , Xu Sun