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Related papers: The TOTEM nT2 detector: architecture, operation an…

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Technology developed for the T2K electromagnetic calorimeter has been adapted to make a small footprint, reliable, segmented detector to characterise anti-neutrinos emitted by nuclear reactors. The device has been developed and demonstrated…

Instrumentation and Detectors · Physics 2018-11-05 J. Carroll , J. Coleman , G. Davies , M. Lockwood , C. Metelko , R. Mills , M. Murdoch , A. Roberts , Y. Schnellbach , C. Touramanis

The SIDDHARTA-2 collaboration at the INFN Laboratories of Frascati (LNF) aims to perform groundbreaking measurements on kaonic atoms. In parallel and beyond the ongoing kaonic deuterium, presently running on the DA$\Phi$NE collider at LNF,…

A 760 $\times$ 760 $\times$ 30 mm$^3$ plastic scintillation detector viewed by photomultiplier tubes (PMTs) from four corners has been developed, and the detector has been tested with cosmic rays and $\gamma$ rays. A position-independent…

Instrumentation and Detectors · Physics 2016-08-03 Shu-wen Tang , Yu-hong Yu , Yong Zhou , Zhi-yu Sun , Xue-heng Zhang , Shi-tao Wang , Ke Yue , Long-xiang Liu , Fang Fang , Duo Yan , Yu Sun , Zhao-min Wang

The CMS detector will be upgraded for the HL-LHC to include a MIP Timing Detector (MTD). The MTD will consist of barrel and endcap timing layers, BTL and ETL respectively, providing precision timing of charged particles. The BTL sensors are…

The Wendelstein 7-X (W7-X) Thomson scattering (TS) diagnostic was upgraded to transiently achieve kilohertz sampling rates combined with adjustable measuring times. The existing Nd:YAG lasers are employed to repetitively emit "bursts", i.e.…

Smart contracts are programs stored and executed on a blockchain. The Ethereum platform, an open-source blockchain-based platform, has been designed to use these programs offering secured protocols and transaction costs reduction. The…

Computational Engineering, Finance, and Science · Computer Science 2019-05-27 Jeremy Charlier , Radu State , Jean Hilger

A new near detector, SciBar, for the K2K long-baseline neutrino oscillation expe riment was installed to improve the measurement of neutrino energy spectrum and to study neutrino interactions in the energy region around 1 GeV. SciBar is a…

High Energy Physics - Experiment · Physics 2015-06-25 K. Nitta

The Tile Calorimeter (TileCal) is a sampling hadronic calorimeter covering the central region of the ATLAS experiment. TileCal uses steel as absorber and plastic scintillators as active medium. The scintillators are read-out by the…

Instrumentation and Detectors · Physics 2021-05-20 Merve Nazlim Agaras

With the installation of the T1 telescope and the Roman Pot stations at 147 m from IP5, the detector apparatus of the TOTEM experiment has been completed during the technical stop in winter 2010/2011. After the commissioning of the…

High Energy Physics - Experiment · Physics 2019-08-28 M. Deile

We consider diffractive processes which can be measured at the LHC. Analysis of diffractive events will give unique information about the high energy asymptotics of hadron scattering. In semihard diffraction one may study the partonic…

High Energy Physics - Phenomenology · Physics 2017-08-23 M. G. Ryskin , A. D. Martin , V. A. Khoze

A new high-granular compact time-of-flight neutron detector for the identification and energy measurement of neutrons produced in nucleus-nucleus interactions at the BM@N experiment, Dubna, Russia, at energies up to 4 AGeV is under…

Instrumentation and Detectors · Physics 2024-08-19 N. Karpushkin , D. Finogeev , F. Guber , D. Lyapin , A. Makhnev , S. Morozov , D. Serebryakov

The Large Hadron Collider (LHC) at CERN is expected to be upgraded to the High-Luminosity LHC (HL-LHC) by 2029 and achieve instantaneous luminosity around 5 - 7.5 $\times$ 10$^{34}$cm$^{-2}$ s$^{-1}$. This represents a more than 3-4 fold…

We present the development of the miniTimeCube (mTC), a novel compact neutrino detector. The mTC is a multipurpose detector, aiming to detect not only neutrinos but also fast/thermal neutrons. Potential applications include the…

The T2K experiment widely uses plastic scintillator as a target for neutrino interactions and an active medium for the measurement of charged particles produced in neutrino interactions at its near detector complex. Over 10 years of…

Instrumentation and Detectors · Physics 2022-07-27 The T2K Collaboration , K. Abe , N. Akhlaq , R. Akutsu , A. Ali , C. Alt , C. Andreopoulos , M. Antonova , S. Aoki , T. Arihara , Y. Asada , Y. Ashida , E. T. Atkin , S. Ban , M. Barbi , G. J. Barker , G. Barr , D. Barrow , M. Batkiewicz-Kwasniak , F. Bench , V. Berardi , L. Berns , S. Bhadra , A. Blanchet , A. Blondel , S. Bolognesi , T. Bonus , S. Bordoni , S. B. Boyd , A. Bravar , C. Bronner , S. Bron , A. Bubak , M. Buizza Avanzini , N. F. Calabria , S. Cao , A. J. Carter , S. L. Cartwright , M. G. Catanesi , A. Cervera , J. Chakrani , D. Cherdack , G. Christodoulou , M. Cicerchia , J. Coleman , G. Collazuol , L. Cook , A. Cudd , Yu. I. Davydov , A. De Roeck , G. De Rosa , T. Dealtry , C. C. Delogu , C. Densham , A. Dergacheva , F. Di Lodovico , S. Dolan , D. Douqa , T. A. Doyle , O. Drapier , K. E. Duffy , J. Dumarchez , P. Dunne , K. Dygnarowicz , A. Eguchi , S. Emery-Schrenk , A. Ershova , S. Fedotov , P. Fernandez , A. J. Finch , G. A. Fiorentini Aguirre , G. Fiorillo , M. Friend , Y. Fujii , Y. Fukuda , K. Fusshoeller , C. Giganti , V. Glagolev , M. Gonin , E. A. G. Goodman , A. Gorin , M. Grassi , M. Guigue , D. R. Hadley , J. T. Haigh , P. Hamacher-Baumann , D. A. Harris , M. Hartz , T. Hasegawa , S. Hassani , N. C. Hastings , A. Hatzikoutelis , Y. Hayato , A. Hiramoto , M. Hogan , J. Holeczek , A. Holin , T. J. Holvey , N. T. Hong Van , T. Honjo , F. Iacob , A. K. Ichikawa , M. Ikeda , T. Ishida , M. Ishitsuka , H. T. Israel , K. Iwamoto , A. Izmaylov , N. Izumi , M. Jakkapu , B. Jamieson , S. J. Jenkins , C. Jesús-Valls , J. J. Jiang , P. Jonsson , C. K. Jung , P. B. Jurj , M. Kabirnezhad , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , S. P. Kasetti , Y. Kataoka , Y. Katayama , T. Katori , M. Kawaue , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , H. Kikutani , S. King , J. Kisiel , A. Knight , T. Kobata , T. Kobayashi , L. Koch , G. Kogan , A. Konaka , L. L. Kormos , Y. Koshio , A. Kostin , K. Kowalik , Y. Kudenko , S. Kuribayashi , R. Kurjata , T. Kutter , M. Kuze , M. La Commara , L. Labarga , J. Lagoda , S. M. Lakshmi , M. Lamers James , I. Lamont , M. Lamoureux , D. Last , N. Latham , M. Laveder , M. Lawe , Y. Lee , C. Lin , T. Lindner , S. -K. Lin , R. P. Litchfield , S. L. Liu , A. Longhin , K. R. Long , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , M. Malek , M. Mandal , S. Manly , A. D. Marino , L. Marti-Magro , D. G. R. Martin , M. Martini , J. F. Martin , T. Maruyama , T. Matsubara , V. Matveev , C. Mauger , K. Mavrokoridis , E. Mazzucato , N. McCauley , J. McElwee , K. S. McFarland , C. McGrew , A. Mefodiev , G. D. Megias , L. Mellet , C. Metelko , M. Mezzetto , A. Minamino , O. Mineev , S. Mine , M. Miura , L. Molina Bueno , S. Moriyama , Th. A. Mueller , D. Munford , L. Munteanu , K. Nagai , Y. Nagai , T. Nakadaira , K. Nakagiri , M. Nakahata , Y. Nakajima , A. Nakamura , H. Nakamura , K. Nakamura , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , T. V. Ngoc , V. Q. Nguyen , K. Niewczas , Y. Nishimura , K. Nishizaki , F. Nova , P. Novella , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , T. Odagawa , T. Ogawa , R. Okada , K. Okumura , T. Okusawa , R. A. Owen , Y. Oyama , V. Palladino , V. Paolone , M. Pari , J. Parlone , S. Parsa , J. Pasternak , M. Pavin , D. Payne , G. C. Penn , D. Pershey , L. Pickering , C. Pidcott , G. Pintaudi , C. Pistillo , B. Popov , K. Porwit , M. Posiadala-Zezula , Y. S. Prabhu , B. Quilain , T. Radermacher , E. Radicioni , B. Radics , P. N. Ratoff , M. Reh , C. Riccio , E. Rondio , S. Roth , A. Rubbia , A. C. Ruggeri , C. A. Ruggles , A. Rychter , K. Sakashita , F. Sánchez , G. Santucci , C. M. Schloesser , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , A. Shaikhiev , A. Shaykina , M. Shiozawa , W. Shorrock , A. Shvartsman , K. Skwarczynski , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , Y. Sonoda , R. Spina , H. Su , I. A. Suslov , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , A. A. Sztuc , M. Tada , S. Takayasu , A. Takeda , Y. Takeuchi , H. K. Tanaka , Y. Tanihara , M. Tani , V. V. Tereshchenko , N. Teshima , N. Thamm , L. F. Thompson , W. Toki , C. Touramanis , T. Towstego , K. M. Tsui , T. Tsukamoto , M. Tzanov , Y. Uchida , A. Vacheret , M. Vagins , D. Vargas , G. Vasseur , C. Vilela , W. G. S. Vinning , T. Vladisavljevic , T. Wachala , J. G. Walsh , Y. Wang , L. Wan , D. Wark , M. O. Wascko , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , K. Wood , C. Wret , J. Xia , Y. -h. Xu , K. Yamamoto , C. Yanagisawa , G. Yang , T. Yano , K. Yasutome , N. Yershov , U. Yevarouskaya , M. Yokoyama , Y. Yoshimoto , M. Yu , R. Zaki , A. Zalewska , J. Zalipska , K. Zaremba , G. Zarnecki , X. Zhao , T. Zhu , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos

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 event rates for WIMP-nucleus and neutrino-nucleus scattering processes, expected to be detected in ton-scale rare-event detectors, are investigated. We focus on nuclear isotopes that correspond to the target nuclei of current and future…

Nuclear Theory · Physics 2020-09-16 R. Sahu , D. K. Papoulias , V. K. B. Kota , T. S. Kosmas

The performance of a scintillating fiber detector prototype for tracking under high rate conditions is investigated. A spatial resolution of about100 micron is aimed for the detector. Further demands are low occupancy and radiation hardness…

High Energy Physics - Experiment · Physics 2007-05-23 E. C. Aschenauer , J. Baehr , V. Gapienko , B. Hoffmann , A. Kharchilava , H. Luedecke , R. Nahnhauer , R. Shanidze

During the high-luminosity phase of the LHC (HL-LHC), planned to start around 2027, the accelerator is expected to deliver an instantaneous peak luminosity of up to $7.5\times10^{34}$ cm$^{-2}$s$^{-1}$. A total integrated luminosity of…

Instrumentation and Detectors · Physics 2020-06-17 The Tracker Group of the CMS Collaboration

The Tile Calorimeter at ATLAS is a hadron calorimeter based on steel plates and scintillating tiles read out by PMTs. The current read-out system uses standard ADCs and custom ASICs to digitize and temporarily store the data on the…

Instrumentation and Detectors · Physics 2015-10-28 Henrik Åkerstedt , Steffen Muschter , Gary Drake , Kelby Anderson , Christian Bohm , Mark Oreglia , Fukun Tang

The LIDAR Thomson scattering concept was proposed in 1983 and then implemented for the first time on the JET tokamak in 1987. A number of modifications were performed and published in 1995, but since then no major changes were made for…

Instrumentation and Detectors · Physics 2013-12-12 M Maslov , M N A Beurskens , M Kempenaars , J Flanagan , JET EFDA contributors