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Liquid-metal jet X-ray sources promise to deliver high photon fluxes, which are unprecedented for laboratory based X-ray sources, because the regenerating liquid-metal anode is less sensitive to damage caused by an increased electron beam…

Instrumentation and Detectors · Physics 2019-05-24 Malte Wansleben , Claudia Zech , Cornelia Streeck , Jan Weser , Christoph Genzel , Burkhard Beckhoff , Roland Mainz

In this paper, we present an investigation into the scintillation properties and pulse shape discrimination (PSD) performance of the new BSO-406, which is a blend of 40% organic glass scintillator and 60% polystyrene. We tested a…

A light yield of 20.4 $\pm$ 0.8 photoelectrons/keV was achieved with an undoped CsI crystal coupled directly to a photomultiplier tube at 77 Kelvin. This is by far the largest yield in the world achieved with CsI crystals. An energy…

Instrumentation and Detectors · Physics 2016-10-06 Jing Liu , Masaki Yamashita , Arun Kumar Soma

Light power spectra are introduced as a new tool for relative light yield (LY) determinations. Light event spectra have commonly been used for this purpose. Theoretical background supporting this change is provided. It is shown that the…

Instrumentation and Detectors · Physics 2019-02-20 J. B. Cumming , S. Hans , M. Yeh

We present new measurements of the scintillation and ionization yields in liquid xenon for low energy electronic (about 3--7 keV$_{ee}$) and nuclear recoils (about 8--20 keV$_{nr}$) at different drift fields from 236 V/cm to 3.93 kV/cm,…

Instrumentation and Detectors · Physics 2015-08-19 Qing Lin , Jialing Fei , Fei Gao , Jie Hu , Yuehuan Wei , Xiang Xiao , Hongwei Wang , Kaixuan Ni

Silicon photomultipliers (SiPMs) are a good alternative to photomultiplier tubes (PMTs) because their gain and quantum efficiency are comparable to PMTs. However, the largest single-chip SiPM is still less than 1~cm$^2$. In order to use…

Instrumentation and Detectors · Physics 2017-11-17 Felix Liang , Hartmut Brands , Les Hoy , Jeff Preston , Jason Smith

To investigate the 1.6 GeV high-energy proton beam detector utilized in the CSNS Phase-II upgrade project, a plastic scintillator detector presents a viable option due to its superior radiation hardness. This study investigates the effects…

Instrumentation and Detectors · Physics 2023-09-11 Yue Zhang , Ruirui Fan , Yuhong Yu , Hantao Jing , Zhixin Tan , Yuhang Guo , You Lv

Benchmarking simulation codes for electron transport and scattering in matter is a crucial step for estimating uncertainties in many applications. However, experimental data for electron energies of a few MeV is scarce to make such…

As a prototype detector for the SHiP Surrounding Background Tagger (SBT), we constructed a cell (120 cm x 80 cm x 25 cm) made from corten steel that is filled with liquid scintillator (LS) composed of linear alkylbenzene (LAB) and…

We present preliminary results on efficiency and light collection uniformity read out performances of different assemblies of scintillator tiles, coupled with solid state photon detectors of different make. Our test beam data suggest that…

Instrumentation and Detectors · Physics 2009-01-14 A. Calcaterra , R. de Sangro , G. Finocchiaro , E. Kuznetsova , P. Patteri , M. Piccolo

In this manuscript we report on the scintillation properties and pulse shape discrimination (PSD) performance of new organic glass scintillator. Two cylindrical samples with dimensions of 2x2 inches were tested. Additionally, this two…

Prototype scintilator+WLS strips with SiPM readout for large muon detection systems were tested in the muon beam of the Fermilab Test Beam Facility. Light yield of up to 137 photoelectrons per muon per strip has been observed, as well as…

Instrumentation and Detectors · Physics 2017-01-03 Dmitri Denisov , Valery Evdokimov , Strahinja Lukić , Predrag Ujić

Plastic scintillators are widely used in high-energy and medical physics, often for measuring the energy of ionizing radiation. Their main disadvantage is their non-linear response to highly ionizing radiation, called ionization quenching.…

Instrumentation and Detectors · Physics 2021-02-03 Thomas Pöschl , Daniel Greenwald , Martin Jan Losekamm , Stephan Paul

Nonlinear Compton scattering is the process of emission of a single photon by a charge driven by an intense laser field. Here, we study the infrared behavior of the photon yield emitted via nonlinear Compton scattering. We first consider…

High Energy Physics - Phenomenology · Physics 2026-05-25 Antonino Di Piazza , Giulio Audagnotto

Results of the measurements with cosmic muons for the light yield of 2-meter long extruded scintillation bar (strip) as a function of distance for different options for light collection technique are presented. Scintillation strip cross…

For the calorimetric determination of the primary energy of extensive air showers, measured by fluorescence telescopes, a precise knowledge of the conversion factor (fluorescence yield) between the deposited energy in the atmosphere and the…

Astrophysics · Physics 2009-06-23 Tilo Waldenmaier , Johannes Blümer , Hans Klages

Radiation damage of J-series silicon photomultipliers (SiPMs) has been studied in the context of using these photodetectors in future space-borne scintillation detectors. Several SiPM samples were exposed to 101.4 MeV protons, with 1 MeV…

The $3 \times 1 \times 1$ m$^3$ demonstrator is a dual phase liquid argon time projection chamber that has recorded cosmic rays events in 2017 at CERN. The light signal in these detectors is crucial to provide precise timing capabilities.…

Instrumentation and Detectors · Physics 2021-03-24 B. Aimard , L. Aizawa , C. Alt , J. Asaadi , M. Auger , V. Aushev , D. Autiero , A. Balaceanu , G. Balik , L. Balleyguier , E. Bechetoille , D. Belver , A. M. Blebea-Apostu , S. Bolognesi , S. Bordoni , N. Bourgeois , B. Bourguille , J. Bremer , G. Brown , G. Brunetti , L. Brunetti , D. Caiulo , M. Calin , E. Calvo , M. Campanelli , K. Cankocak , C. Cantini , B. Carlus , B. M. Cautisanu , M. Chalifour , A. Chappuis , N. Charitonidis , A. Chatterjee , A. Chiriacescuf , P. Chiu , S. Conforti , P. Cotte , P. Crivelli , C. Cuesta , J. Dawson , I. De Bonis , C. De La Taille , A. Delbart , S. Di Luise , F. Doizon , C. Drancourt , D. Duchesneau , F. Dulucq , F. Duval , S. Emery , A. Ereditato , A. Falcone , K. Fusshoeller , A. Gallego-Ros , V. Galymov , N. Geffroy , A. Gendotti , A. Gherghel-Lascu , I. Gil-Botella , C. Girerd , M. C. Gomoiu , P. Gorodetzky , E. Hamada , R. Hanni , T. Hasegawa , A. Holin , S. Horikawa , M. Ikeno , S. Jiménez , A. Jipa , M. Karolak , Y. Karyotakis , S. Kasai , K. Kasami , T. Kishishita , H. Konari , I. Kreslo , D. Kryn , P. Kunzé , M. Kurokawa , Y. Kuromori , C. Lastoria , I. Lazanu , G. Lehmann-Miotto , M. Leyton , N. Lira , K. Loo , D. Lorca , P. Lutz , T. Lux , J. Maalampi , G. Maire , M. Maki , L. Manenti , R. M. Margineanu , J. Marteau , G. Martin-Chassard , H. Mathez , E. Mazzucato , G. Misitano , D. Mladenov , L. Molina Bueno , T. S. Mosu , W. Mu , S. Murphy , K. Nakayoshi , S. Narita , D. Navas-Nicolás , K. Negishi , M. Nessi , M. Niculescu-Oglinzanu , F. Noto , A. Noury , Y. Onishchuk , C. Palomares , M. Parvu , T. Patzak , Y. Penichot , E. Pennacchio , L. Periale , H. Pessard , F. Pietropaolo , D. Pugnere , B. Radics , D. Redondo , C. Regenfus , A. Remoto , F. Resnati , O. Ristea , A. Rubbia , A. Saftoiu , K. Sakashita , F. Sanchez , C. Santos , A. Scarpelli , C. Schloesser , K. Sendai , F. Sergiampietri , S. Shahsavarani , M. Shoji , J. Sinclair , J. Soto-Oton , D. I. Stanca , D. Stefan , R. Sulej , M. Tanaka , V. Toboaru , A. Tonazzo , W. Tromeur , W. H. Trzaska , T. Uchida , L. Urda , F. Vannucci , G. Vasseur , A. Verdugo , T. Viant , S. Vihonen , S. Vilalte , M. Weber , S. Wu , J. Yu , L. Zambelli , M. Zito
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