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

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Monolithic CMOS pixel detectors have emerged as competitive contenders in the field of high-energy particle physics detectors. By utilizing commercial processes they offer high-volume production of such detectors. A series of prototypes has…

The apparatus of the ALICE experiment at CERN will be upgraded in 2017/18 during the second long shutdown of the LHC (LS2). A major motivation for this upgrade is to extend the physics reach for charmed and beauty particles down to low…

The ALICE experiment at CERN is undergoing a major upgrade during the Long Shutdown 2 (LS2) of the LHC during 2019-2020. The key elements regarding the central barrel are the installation of a new Inner Tracking System (ITS) and the upgrade…

Instrumentation and Detectors · Physics 2021-02-03 Felix Reidt

In the high luminosity era of the Large Hadron Collider, the HL-LHC, the instantaneous luminosity is expected to reach unprecedented values, resulting in about 200 proton-proton interactions in a typical bunch crossing. To cope with the…

The LHC generates an intense beam of high-energy neutrinos in the forward direction, whose scientific potential has been left unexploited for many years. The FASER and SND@LHC experiments, operating since 2023, have recently measured LHC…

High Energy Physics - Phenomenology · Physics 2025-10-30 Peter Krack

ALDO2 is a multi-function, adjustable, low dropout linear regulator designed in onsemi I3T80 0.35~$\mu$m HV CMOS technology for use in HEP detectors that adopt silicon photomultipliers (SiPMs). The chip features four independent regulators,…

Instrumentation and Detectors · Physics 2022-08-31 Paolo Carniti , Claudio Gotti , Gianluigi Pessina

The feasibility studies of the measurement of the central exclusive jet production at the LHC using the proton tagging technique are presented. In order to reach the low jet-mass region, single tagged events were considered. The studies…

High Energy Physics - Phenomenology · Physics 2015-08-10 M. Trzebinski , R. Staszewski , J. Chwastowski

A precise and efficient tracking is one of the critical components of the CMS physics program as it impacts the ability to reconstruct the physics objects needed to understand proton-proton collisions at the LHC. The CMS detector has…

High Energy Physics - Experiment · Physics 2023-12-14 Walaa Elmetenawee

Strong multiple scattering of the probe in scanning transmission electron microscopy (STEM) means image simulations are usually required for quantitative interpretation and analysis of elemental maps produced by electron energy-loss…

Materials Science · Physics 2019-12-25 Hamish G. Brown , Jim Ciston , Colin Ophus

In the context of particle therapy monitoring, we are developing a gamma-ray detector to determine the ion range in vivo from the measurement of particle time-of-flight. For this application, a beam monitor capable to tag in time the…

We present the FP420 R&D project, which has been studying the key aspects of the development and installation of a silicon tracker and fast-timing detectors in the LHC tunnel at 420 m from the interaction points of the ATLAS and CMS…

Time-tagging units and coincidence detectors are used in many scientific research fields. The required timing resolution and number of input channels are varying, but some emerging experiments in the field of quantum optics require up to 32…

Instrumentation and Detectors · Physics 2020-11-03 Attila Hidvegi

In this talk we present a selection of forward physics results recently obtained with the run-1 and run-2 LHC data by the CMS, LHCf and TOTEM experiments. The status of the very forward LHC proton spectrometer, CT-PPS, is discussed:…

High Energy Physics - Experiment · Physics 2017-09-01 Mirko Berretti

In this work we present an active Compton scattering polarimeter as a focal plane instrument able to extend the X-ray polarimetry towards hard X-rays. Other authors have already studied various instrument design by means of Monte Carlo…

Instrumentation and Methods for Astrophysics · Physics 2013-01-08 Sergio Fabiani , Riccardo Campana , Enrico Costa , Ettore Del Monte , Fabio Muleri , Alda Rubini , Paolo Soffitta

New measurements from ATLAS at the LHC are presented on the total cross section at $\sqrt{s}=8$ TeV from elastic scattering using the ALFA sub-detector and on the inelastic cross section at $\sqrt{s}=13$ TeV using the MBTS sub-detector.

High Energy Physics - Experiment · Physics 2017-04-05 H. Stenzel

Several LHC experiments exploit the high acceptance in the forward region. Most of them use the possibility of measuring the intact proton in an elastic event. This approach can enhance the purity of selecting jet-gap-jet events, leading to…

High Energy Physics - Experiment · Physics 2024-01-22 Anna Fehérkuti

The T2K experiment is a long-baseline neutrino oscillation experiment. Its main goal is to measure the last unknown lepton sector mixing angle {\theta}_{13} by observing {\nu}_e appearance in a {\nu}_{\mu} beam. It also aims to make a…

Instrumentation and Detectors · Physics 2019-08-14 T2K Collaboration , K. Abe , N. Abgrall , H. Aihara , Y. Ajima , J. B. Albert , D. Allan , P. -A. Amaudruz , C. Andreopoulos , B. Andrieu , M. D. Anerella , C. Angelsen , S. Aoki , O. Araoka , J. Argyriades , A. Ariga , T. Ariga , S. Assylbekov , J. P. A. M. de André , D. Autiero , A. Badertscher , O. Ballester , M. Barbi , G. J. Barker , P. Baron , G. Barr , L. Bartoszek , M. Batkiewicz , F. Bay , S. Bentham , V. Berardi , B. E. Berger , H. Berns , I. Bertram , M. Besnier , J. Beucher , D. Beznosko , S. Bhadra , P. Birney , D. Bishop , E. Blackmore , F. d. M. Blaszczyk , J. Blocki , A. Blondel , A. Bodek , C. Bojechko , J. Bouchez , T. Boussuge , S. B. Boyd , M. Boyer , N. Braam , R. Bradford , A. Bravar , K. Briggs , J. D. Brinson , C. Bronner , D. G. Brook-Roberge , M. Bryant , N. Buchanan , H. Budd , M. Cadabeschi , R. G. Calland , D. Calvet , J. Caravaca Rodríguez , J. Carroll , S. L. Cartwright , A. Carver , R. Castillo , M. G. Catanesi , C. Cavata , A. Cazes , A. Cervera , J. P. Charrier , C. Chavez , S. Choi , S. Chollet , G. Christodoulou , P. Colas , J. Coleman , W. Coleman , G. Collazuol , K. Connolly , P. Cooke , A. Curioni , A. Dabrowska , I. Danko , R. Das , G. S. Davies , S. Davis , M. Day , X. De La Broise , P. de Perio , G. De Rosa , T. Dealtry , A. Debraine , E. Delagnes , A. Delbart , C. Densham , F. Di Lodovico , S. Di Luise , P. Dinh Tran , J. Dobson , J. Doornbos , U. Dore , O. Drapier , F. Druillole , F. Dufour , J. Dumarchez , T. Durkin , S. Dytman , M. Dziewiecki , M. Dziomba , B. Ellison , S. Emery , A. Ereditato , J. E. Escallier , L. Escudero , L. S. Esposito , W. Faszer , M. Fechner , A. Ferrero , A. Finch , C. Fisher , M. Fitton , R. Flight , D. Forbush , E. Frank , K. Fransham , Y. Fujii , Y. Fukuda , M. Gallop , V. Galymov , G. L. Ganetis , F. C. Gannaway , A. Gaudin , J. Gaweda , A. Gendotti , M. George , S. Giffin , C. Giganti , K. Gilje , I. Giomataris , J. Giraud , A. K. Ghosh , T. Golan , M. Goldhaber , J. J. Gomez-Cadenas , S. Gomi , M. Gonin , M. Goyette , A. Grant , N. Grant , F. Grañena , S. Greenwood , P. Gumplinger , P. Guzowski , M. D. Haigh , K. Hamano , C. Hansen , T. Hara , P. F. Harrison , B. Hartfiel , M. Hartz , T. Haruyama , R. Hasanen , T. Hasegawa , N. C. Hastings , S. Hastings , A. Hatzikoutelis , K. Hayashi , Y. Hayato , T. D. J. Haycock , C. Hearty , R. L. Helmer , R. Henderson , S. Herlant , N. Higashi , J. Hignight , K. Hiraide , E. Hirose , J. Holeczek , N. Honkanen , S. Horikawa , A. Hyndman , A. K. Ichikawa , K. Ieki , M. Ieva , M. Iida , M. Ikeda , J. Ilic , J. Imber , T. Ishida , C. Ishihara , T. Ishii , S. J. Ives , M. Iwasaki , K. Iyogi , A. Izmaylov , B. Jamieson , R. A. Johnson , K. K. Joo , G. Jover-Manas , C. K. Jung , H. Kaji , T. Kajita , H. Kakuno , J. Kameda , K. Kaneyuki , D. Karlen , K. Kasami , V. Kasey , I. Kato , H. Kawamuko , E. Kearns , L. Kellet , M. Khabibullin , M. Khaleeq , N. Khan , A. Khotjantsev , D. Kielczewska , T. Kikawa , J. Y. Kim , S. -B. Kim , N. Kimura , B. Kirby , J. Kisiel , P. Kitching , T. Kobayashi , G. Kogan , S. Koike , T. Komorowski , A. Konaka , L. L. Kormos , A. Korzenev , K. Koseki , Y. Koshio , Y. Kouzuma , K. Kowalik , V. Kravtsov , I. Kreslo , W. Kropp , H. Kubo , J. Kubota , Y. Kudenko , N. Kulkarni , L. Kurchaninov , Y. Kurimoto , R. Kurjata , Y. Kurosawa , T. Kutter , J. Lagoda , K. Laihem , R. Langstaff , M. Laveder , T. B. Lawson , P. T. Le , A. Le Coguie , M. Le Ross , K. P. Lee , M. Lenckowski , C. Licciardi , I. T. Lim , T. Lindner , R. P. Litchfield , A. Longhin , G. D. Lopez , P. Lu , L. Ludovici , T. Lux , M. Macaire , L. Magaletti , K. Mahn , Y. Makida , C. J. Malafis , M. Malek , S. Manly , A. Marchionni , C. Mark , A. D. Marino , A. J. Marone , J. Marteau , J. F. Martin , T. Maruyama , T. Maryon , J. Marzec , P. Masliah , E. L. Mathie , C. Matsumura , K. Matsuoka , V. Matveev , K. Mavrokoridis , E. Mazzucato , N. McCauley , K. S. McFarland , C. McGrew , T. McLachlan , I. Mercer , M. Messina , W. Metcalf , C. Metelko , M. Mezzetto , P. Mijakowski , C. A. Miller , A. Minamino , O. Mineev , S. Mine , R. E. Minvielle , G. Mituka , M. Miura , K. Mizouchi , J. -P. Mols , L. Monfregola , E. Monmarthe , F. Moreau , B. Morgan , S. Moriyama , D. Morris , A. Muir , A. Murakami , J. F. Muratore , M. Murdoch , S. Murphy , J. Myslik , G. Nagashima , T. Nakadaira , M. Nakahata , T. Nakamoto , K. Nakamura , S. Nakayama , T. Nakaya , D. Naples , B. Nelson , T. C. Nicholls , K. Nishikawa , H. Nishino , K. Nitta , F. Nizery , J. A. Nowak , M. Noy , Y. Obayashi , T. Ogitsu , H. Ohhata , T. Okamura , K. Okumura , T. Okusawa , C. Ohlmann , K. Olchanski , R. Openshaw , S. M. Oser , M. Otani , R. A. Owen , Y. Oyama , T. Ozaki , M. Y. Pac , V. Palladino , V. Paolone , P. Paul , D. Payne , G. F. Pearce , C. Pearson , J. D. Perkin , M. Pfleger , F. Pierre , D. Pierrepont , P. Plonski , P. Poffenberger , E. Poplawska , B. Popov , M. Posiadala , J. -M. Poutissou , R. Poutissou , R. Preece , P. Przewlocki , W. Qian , J. L. Raaf , E. Radicioni , K. Ramos , P. Ratoff , T. M. Raufer , M. Ravonel , M. Raymond , F. Retiere , D. Richards , J. -L. Ritou , A. Robert , P. A. Rodrigues , E. Rondio , M. Roney , M. Rooney , D. Ross , B. Rossi , S. Roth , A. Rubbia , D. Ruterbories , R. Sacco , S. Sadler , K. Sakashita , F. Sanchez , A. Sarrat , K. Sasaki , P. Schaack , J. Schmidt , K. Scholberg , J. Schwehr , M. Scott , D. I. Scully , Y. Seiya , T. Sekiguchi , H. Sekiya , G. Sheffer , M. Shibata , Y. Shimizu , M. Shiozawa , S. Short , M. Siyad , D. Smith , R. J. Smith , M. Smy , J. Sobczyk , H. Sobel , S. Sooriyakumaran , M. Sorel , J. Spitz , A. Stahl , P. Stamoulis , O. Star , J. Statter , L. Stawnyczy , J. Steinmann , J. Steffens , B. Still , M. Stodulski , J. Stone , C. Strabel , T. Strauss , R. Sulej , P. Sutcliffe , A. Suzuki , K. Suzuki , S. Suzuki , S. Y. Suzuki , Y. Suzuki , Y. Suzuki , J. Swierblewski , T. Szeglowski , M. Szeptycka , R. Tacik , M. Tada , A. S. Tadepalli , M. Taguchi , S. Takahashi , A. Takeda , Y. Takenaga , Y. Takeuchi , H. A. Tanaka , K. Tanaka , M. Tanaka , M. M. Tanaka , N. Tanimoto , K. Tashiro , I. J. Taylor , A. Terashima , D. Terhorst , R. Terri , L. F. Thompson , A. Thorley , M. Thorpe , W. Toki , T. Tomaru , Y. Totsuka , C. Touramanis , T. Tsukamoto , V. Tvaskis , M. Tzanov , Y. Uchida , K. Ueno , M. Usseglio , A. Vacheret , M. Vagins , J. F. Van Schalkwyk , J. -C. Vanel , G. Vasseur , O. Veledar , P. Vincent , T. Wachala , A. V. Waldron , C. W. Walter , P. J. Wanderer , M. A. Ward , G. P. Ward , D. Wark , D. Warner , M. O. Wascko , A. Weber , R. Wendell , J. Wendland , N. West , L. H. Whitehead , G. Wikström , R. J. Wilkes , M. J. Wilking , Z. Williamson , J. R. Wilson , R. J. Wilson , K. Wong , T. Wongjirad , S. Yamada , Y. Yamada , A. Yamamoto , K. Yamamoto , Y. Yamanoi , H. Yamaoka , C. Yanagisawa , T. Yano , S. Yen , N. Yershov , M. Yokoyama , A. Zalewska , J. Zalipska , K. Zaremba , M. Ziembicki , E. D. Zimmerman , M. Zito , J. Zmuda

A NaI(Tl) detector array called DALI2 (Detector Array for Low Intensity radiation 2) has been constructed for in-beam $\gamma$-ray spectroscopy experiments with fast radioactive isotope (RI) beams. It consists typically of 186 NaI(Tl)…

Nuclear Experiment · Physics 2014-07-30 S. Takeuchi , T. Motobayashi , Y. Togano , M. Matsushita , N. Aoi , K. Demichi , H. Hasegawa , H. Murakami

The Scattering and Neutrino Detector at the LHC (\SND) started taking data at the beginning of Run 3 of the LHC. The experiment is designed to perform measurements with neutrinos produced in proton-proton collisions at the LHC in an energy…

High Energy Physics - Experiment · Physics 2023-11-17 LHC Collaboration
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