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Nuclear and high energy physics research has a need for new, high performance scintillators with high light yields; high densities, fast decay times, and are radiation hard. In this paper we present crystal growth and results from 16-mm…

Instrumentation and Detectors · Physics 2021-05-03 R. Hawrami , E. Ariesanti , A. Burger , H. Parkhe

The expected increase of total integrated luminosity by a factor of ten at the HL-LHC compared to the design goals for LHC essentially eliminates the safety factor for radiation hardness realized at the current cold amplifiers of the ATLAS…

Instrumentation and Detectors · Physics 2019-08-13 Martin Nagel

The CMS detector at the LHC requires a major upgrade to cope with the higher instantaneous luminosity and the elevated radiation levels. The active media of the forward backing hadron calorimeters is projected to be radiation-hard, high…

Instrumentation and Detectors · Physics 2015-10-30 Emrah Tiras

This report overviews studies accomplished in the U70 proton synchrotron of IHEP-Protvino during the recent two decades. Major attention is paid to a routine application of bent crystals for beam extraction from the machine. It has been…

Cerium-doped Cs$_2$LiYCl$_6$ (CLYC) and Cs$_2$LiLaBr$_x$Cl$_{6-x}$ (CLLBC) are scintillators in the elpasolite family that are attractive options for resource-constrained applications due to their ability to detect both gamma rays and…

Instrumentation and Detectors · Physics 2019-10-23 K. E. Mesick , K. D. Bartlett , D. D. S. Coupland , L. C. Stonehill

A prototype for a sampling calorimeter made out of cerium fluoride crystals interleaved with tungsten plates, and read out by wavelength-shifting fibres, has been exposed to beams of electrons with energies between 20 and 150 GeV, produced…

Crystals are used as a homogeneous calorimetric medium in many high-energy physics experiments. For some experiments, performance has to be ensured in very difficult operating conditions, like a high radiation environment, very large…

Instrumentation and Detectors · Physics 2009-11-10 Francesca Nessi-Tedaldi

The Large Hadron Collider (LHC) at CERN will provide proton-proton collisions at a centre-of-mass energy of 14 TeV with a design luminosity of 10**34/cm**2/s. The exploitation of the rich physics potential offered by the LHC will be…

High Energy Physics - Experiment · Physics 2007-05-23 Felicitas Pauss , Michael Dittmar

We discuss the results of a proton irradiation campaign of a GAGG:Ce (Cerium-doped Gadolinium Aluminium Gallium Garnet) scintillation crystal, carried out in the framework of the HERMES-TP/SP (High Energy Rapid Modular Ensemble of…

Cs$_2$LiYCl$_6$:Ce$^{3+}$ (CLYC) is a new scintillator that is an attractive option for applications requiring the ability to detect both gamma rays and neutrons within a single volume. It is therefore of interest in applications that…

Instrumentation and Detectors · Physics 2018-10-16 K. E. Mesick , D. D. S. Coupland , S. F. Nowicki , L. C. Stonehill

We report the scintillation and timing performance of a new developed 200 * 20 mm * 20 mm large size barium fluoride crystal doped with 3at% yttrium (BaF2:Y) to enhance the application for high time resolution. This doping effectively…

Instrumentation and Detectors · Physics 2025-02-24 Zeyu Huang , Jing Zhang , Shiming Zou , Mingkuan Yuan , Jiawei Xu , Xiyang Wang , Shiqing Xie , Jinhui Chen , Junfeng Chen , Xiaolong Wang

Physical possibility for bending the LHC protons (or ions) a huge angle of 1-20 degrees in the energy range of 0.45 to 7 TeV by means of a bent channeling crystal of Silicon or Germanium is demonstrated. Such an application can be useful…

High Energy Physics - Experiment · Physics 2007-05-23 V. M. Biryukov

The scintillating properties of active materials used in high energy and particle physics experiments play an important role regarding the performances of both calorimeters and experiments. Two scintillator materials, a scintillating glass…

Instrumentation and Detectors · Physics 2018-09-11 Güral Aydın

In view of the implementation of beam-monitoring sensors for CERN's Large Hadron Collider (LHC), and also in order to validate Thermoluminescence Detectors as a versatile tool to measure ionizing radiation doses in mixed fields at hadron…

Instrumentation and Detectors · Physics 2016-09-08 Christoph Ilgner , Maciej Budzanowski , Barbara Obryk

Showers produced by positive hadrons in the highly granular CALICE scintillator-steel analogue hadron calorimeter were studied. The experimental data were collected at CERN and FNAL for single particles with initial momenta from 10 to 80…

Instrumentation and Detectors · Physics 2015-05-20 The CALICE Collaboration , B. Bilki , J. Repond , L. Xia , G. Eigen , M. A. Thomson , D. R. Ward , D. Benchekroun , A. Hoummada , Y. Khoulaki , S. Chang , A. Khan , D. H. Kim , D. J. Kong , Y. D. Oh , G. C. Blazey , A. Dyshkant , K. Francis , J. G. R. Lima , R. Salcido , V. Zutshi , F. Salvatore , K. Kawagoe , Y. Miyazaki , Y. Sudo , T. Suehara , T. Tomita , H. Ueno , T. Yoshioka , J. Apostolakis , D. Dannheim , G. Folger , V. Ivantchenko , W. Klempt , A. -I. Lucaci-Timoce , A. Ribon , D. Schlatter , E. Sicking , V. Uzhinskiy , J. Giraud , D. Grondin , J. -Y. Hostachy , L. Morin , E. Brianne , U. Cornett , D. David , A. Ebrahimi , G. Falley , K. Gadow , P. Göttlicher , C. Günter , O. Hartbrich , B. Hermberg , S. Karstensen , F. Krivan , K. Krüger , S. Lu , B. Lutz , S. Morozov , V. Morgunov , C. Neubüser , M. Reinecke , F. Sefkow , P. Smirnov , H. L. Tran , P. Buhmann , E. Garutti , S. Laurien , M. Matysek , M. Ramilli , K. Briggl , P. Eckert , T. Harion , Y. Munwes , H. -Ch. Schultz-Coulon , W. Shen , R. Stamen , E. Norbeck , D. Northacker , Y. Onel , B. van Doren , G. W. Wilson , M. Wing , C. Combaret , L. Caponetto , R. Eté , G. Grenier , R. Han , J. C. Ianigro , R. Kieffer , I. Laktineh , N. Lumb , H. Mathez , L. Mirabito , A. Petrukhin , A. Steen , J. Berenguer Antequera , E. Calvo Alamillo , M. -C. Fouz , J. Marin , J. Puerta-Pelayo , A. Verdugo , F. Corriveau , B. Bobchenko , R. Chistov , M. Chadeeva , M. Danilov , A. Drutskoy , A. Epifantsev , O. Markin , D. Mironov , R. Mizuk , E. Novikov , V. Rusinov , E. Tarkovsky , D. Besson , P. Buzhan , A. Ilyin , E. Popova , M. Gabriel , C. Kiesling , N. van der Kolk , F. Simon , C. Soldner , M. Szalay , M. Tesar , L. Weuste , M. S. Amjad , J. Bonis , S. Callier , S. Conforti di Lorenzo , P. Cornebise , F. Dulucq , J. Fleury , T. Frisson , G. Martin-Chassard , R. Pöschl , L. Raux , F. Richard , J. Rouëné , N. Seguin-Moreau , Ch. de la Taille , M. Anduze , V. Boudry , J-C. Brient , C. Clerc , R. Cornat , M. Frotin , F. Gastaldi , A. Matthieu , P. Mora de Freitas , G. Musat , M. Ruan , H. Videau , J. Zacek , J. Cvach , P. Gallus , M. Havranek , M. Janata , J. Kvasnicka , D. Lednicky , M. Marcisovsky , I. Polak , J. Popule , L. Tomasek , M. Tomasek , P. Sicho , J. Smolik , V. Vrba , J. Zalesak , D. Jeans , S. Weber

Lepton colliders are considered as options to complement and to extend the physics programme at the Large Hadron Collider. The Compact Linear Collider (CLIC) is an $e^+e^-$ collider under development aiming at centre-of-mass energies of up…

Instrumentation and Detectors · Physics 2014-01-14 C. Adloff , J. -J. Blaising , M. Chefdeville , C. Drancourt , R. Gaglione , N. Geffroy , Y. Karyotakis , I. Koletsou , J. Prast , G. Vouters , J. Repond , J. Schlereth , J. Smith , L. Xia , E. Baldolemar , J. Li , S. T. Park , M. Sosebee , A. P. White , J. Yu , G. Eigen , M. A. Thomson , D. R. Ward , D. Benchekroun , A. Hoummada , Y. Khoulaki , J. Apostolakis , D. Dannheim , A. Dotti , K. Elsener , G. Folger , C. Grefe , V. Ivantchenko , M. Killenberg , W. Klempt , E. van der Kraaij , C. B. Lam , L. Linssen , A. -I. Lucaci-Timoce , A. Muennich , S. Poss , A. Ribon , A. Sailer , D. Schlatter , J. Strube , V. Uzhinskiy , C. Carloganu , P. Gay , S. Manen , L. Royer , M. Tytgat , N. Zaganidis , G. C. Blazey , A. Dyshkant , J. G. R. Lima , V. Zutshi , J. -Y. Hostachy , L. Morin , U. Cornett , D. David , A. Ebrahimi , G. Falley , N. Feege , K. Gadow , P. Goettlicher , C. Guenter , O. Hartbrich , B. Hermberg , S. Karstensen , F. Krivan , K. Krueger , S. Lu , B. Lutz , S. Morozov , V. Morgunov , C. Neubueser , M. Reinecke , F. Sefkow , P. Smirnov , M. Terwort , E. Garutti , S. Laurien , I. Marchesini , M. Matysek , M. Ramilli , K. Briggl , P. Eckert , T. Harion , H. -Ch. Schultz-Coulon , W. Shen , R. Stamen , B. Bilki , E. Norbeck , D. Northacker , Y. Onel , G. W. Wilson , K. Kawagoe , Y. Sudo , T. Yoshioka , P. D. Dauncey , M. Wing , F. Salvatore , E. Cortina Gil , S. Mannai , G. Baulieu , P. Calabria , L. Caponetto , C. Combaret , R. Della Negra , G. Grenier , R. Han , J-C. Ianigro , R. Kieffer , I. Laktineh , N. Lumb , H. Mathez , L. Mirabito , A. Petrukhin , A. Steen , W. Tromeur , M. Vander Donckt , Y. Zoccarato , E. Calvo Alamillo , M. -C. Fouz , J. Puerta-Pelayo , F. Corriveau , B. Bobchenko , M. Chadeeva , M. Danilov , A. Epifantsev , O. Markin , R. Mizuk , E. Novikov , V. Popov , V. Rusinov , E. Tarkovsky , N. Kirikova , V. Kozlov , P. Smirnov , Y. Soloviev , D. Besson , P. Buzhan , A. Ilyin , V. Kantserov , V. Kaplin , A. Karakash , E. Popova , V. Tikhomirov , C. Kiesling , K. Seidel , F. Simon , C. Soldner , M. Szalay , M. Tesar , L. Weuste , M. S. Amjad , J. Bonis , S. Callier , S. Conforti di Lorenzo , P. Cornebise , Ph. Doublet , F. Dulucq , J. Fleury , T. Frisson , N. van der Kolk , H. Li , G. Martin-Chassard , F. Richard , Ch. de la Taille , R. Poeschl , L. Raux , J. Rouene , N. Seguin-Moreau , M. Anduze , V. Balagura , V. Boudry , J-C. Brient , R. Cornat , M. Frotin , F. Gastaldi , E. Guliyev , Y. Haddad , F. Magniette , G. Musat , M. Ruan , T. H. Tran , H. Videau , B. Bulanek , J. Zacek , J. Cvach , P. Gallus , M. Havranek , M. Janata , J. Kvasnicka , D. Lednicky , M. Marcisovsky , I. Polak , J. Popule , L. Tomasek , M. Tomasek , P. Ruzicka , P. Sicho , J. Smolik , V. Vrba , J. Zalesak , B. Belhorma , H. Ghazlane , K. Kotera , T. Takeshita , S. Uozumi , S. Chang , A. Khan , D. H. Kim , D. J. Kong , Y. D. Oh , M. Goetze , J. Sauer , S. Weber , C. Zeitnitz

Scintillating LFS-3 and LFS-8 crystals were exposed to a 155 MeV/c proton fluence $\Phi_{p}=(4.4\pm0.4)\cdot10^{12}cm^{-2}$. There was negligible reduction in transmission spectrum of LFS-3 crystal measured in 30 days after irradiation.

Instrumentation and Detectors · Physics 2011-05-26 V. A. Kozlov , S. A. Kutovoi , A. I. Zagumennyi , Yu. D. Zavartsev , M. V. Zavertyaev , A. F. Zerrouk

At the LHC era, the detector systems are operating at the harsh hadronic environment with the unprecedentedly high particle flux. Position sensitive silicon devices are usually positioned at the innermost regions of the experimental setups…

High Energy Physics - Experiment · Physics 2020-02-17 Agnieszka Oblakowska-Mucha , Tomasz Szumlak

This paper presents the design and optimization of a LYSO crystal electromagnetic calorimeter (ECAL) for the DarkSHINE experiment, which aims to search for dark photons as potential mediators of dark forces. The ECAL design was evaluated…

It is known that the alignment of an high-energy e- beam with specific crystal directions leads to a significant increase of the coherent radiation emission. This enhancement can be exploited to create an intense photon source. An elective…