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Based on elastic collisions, the linear momentum of a fast neutron can be measured from as few as two consecutive recoil ion tracks plus the vertex position of the third collision, or `two and half' ion tracks. If the time delay between the…

Instrumentation and Detectors · Physics 2023-08-22 Zhehui Wang , Christopher L. Morris

The central component of the CMS detector is the largest silicon tracker ever built. The precise alignment of this complex device is a formidable challenge, and only achievable with a significant extension of the technologies routinely used…

Instrumentation and Detectors · Physics 2014-08-22 CMS Collaboration

In order to fully exploit the physics potential of a e+e- linear collider, such as TESLA, a Vertex Tracker providing high resolution track reconstruction is required. Hybrid Silicon pixel sensors are an attractive sensor technology option…

High Energy Physics - Experiment · Physics 2007-05-23 M. Battaglia , M. Caccia , S. Borghi , R. Campagnolo , K. Domanski , P. Grabiec , B. Jaroszewicz , J. Marczewski , D. Tomaszewski , W. Kucewicz , A. Zalewska , K. Tammi

The ATLAS Inner Detector is a composite tracking system consisting of silicon pixels, silicon strips and straw tubes in a 2 T magnetic field. Its installation was completed in August 2008 and the detector took part in data- taking with…

Instrumentation and Detectors · Physics 2012-08-27 The ATLAS Collaboration

The first stage of the FCC (Future Circular Collider) is a high-luminosity electron-positron collider (FCC-ee) with centre-of-mass energy ranging from 88 to 365 GeV, to study with high precision the Z, W, Higgs and top particles, with…

The Compact Linear Collider CLIC is designed to deliver e+e- collisions at a center of mass energy of up to 3 TeV. The detector systems at this collider have to provide highly efficient tracking and excellent jet energy resolution and…

Instrumentation and Detectors · Physics 2011-09-16 Frank Simon

The FCC-ee is a proposed future high-energy, high-intensity and high-precision lepton collider. Here, we present the latest development for the FCC-ee interaction regions, which shall ensure optimum conditions for the particle physics…

The FCC-ee phase of a Future Circular Collider is generating great interest due to its versatility, allowing the study of various electroweak thresholds, $Z$, $WW$, $ZH$, and $t \bar{t}$. Electroweak precision physics is complemented by…

High Energy Physics - Phenomenology · Physics 2025-10-28 Luiz Vale Silva

The harsh machine background at the Compact Linear Collider (CLIC) forms a strong constraint on the design of the innermost part of the tracker. For the CLIC Conceptual Design Report, the detector concepts developed for the International…

Instrumentation and Detectors · Physics 2012-03-06 D. Dannheim , A. Sailer , J. Trenado , M. Vos

The future Electron-Ion Collider (EIC) will utilize a series of high-luminosity high-energy electron+proton ($e+p$) and electron+nucleus ($e+A$) collisions to explore the inner structure of nucleon and nucleus and the matter formation…

The Future Circular Collider (FCC) study investigates the feasibility of circular colliders in the post-LHC era. The sub-study FCC-ee is a 100 km electron positron collider in the energy range of 90-365 GeV. In order to achieve a design…

Accelerator Physics · Physics 2021-11-30 Bastian Haerer , Tobias Tydecks

For many years there has been an aspiration within the community to develop curved silicon detectors for particle physics applications. We present the results from 10 x 10cm low mass support modules as a part of the "ZeroMass" project that…

Instrumentation and Detectors · Physics 2025-03-07 Sam Moss , Zhidong Zhang , Adrian Bevan , Mark Bullough , Jens Dopke , Jag Mistry , Seth Zenz

The upgrade of the LHC to the High-Luminosity LHC (HL-LHC) is expected to increase the current instantaneous luminosity by a factor of 5 to 7, providing the opportunity to study rare processes and measure precisely the standard model…

Instrumentation and Detectors · Physics 2020-02-07 Patrick Asenov

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 structure of the CMS inner tracking system has been studied using nuclear interactions of hadrons striking its material. Data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded in 2015 at the LHC are used to…

Instrumentation and Detectors · Physics 2018-11-01 CMS Collaboration

We present results of a study of charged particle track and vertex reconstruction with a beam telescope made of four layers of 50 micron-thin CMOS monolithic pixel sensors using the 120 GeV protons at the FNAL Meson Test Beam Facility. We…

For most physical processes the tracks observed in the muon stations must be matched with the corresponding tracks in the inner tracker, the external muon system providing muon identification and triggering but the tracker points giving the…

High Energy Physics - Experiment · Physics 2016-08-31 A. Benvenuti , D. Denegri , V. Genchev , A. Khanov , N. Stepanov , P. Vankov

CMOS pixel sensors (CPS) represent a novel technological approach to building charged particle detectors. CMOS processes allow to integrate a sensing volume and readout electronics in a single silicon die allowing to build sensors with a…

The ALICE Collaboration is developing a novel vertexing detector to extend the heavy-flavour physics programme of the experiment during Run 4 by improving the pointing resolution of the tracking, particularly at low transverse momentum. It…

Instrumentation and Detectors · Physics 2024-08-05 Domenico Colella

This manuscript is devoted to the description of the proposed Future Circular Collider (FCC) project and its physics program focused on measurements involving heavy quarks. It summarizes the report submitted to the US 2021 Snowmass Process…

High Energy Physics - Experiment · Physics 2022-07-12 Radek Novotny
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