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Chromatic calorimetry (CCAL) analyses particle detection by utilizing scintillators with distinct emission wavelengths to measure the longitudinal energy deposition of particle showers in high-energy physics, improving particle…

High Energy Physics - Experiment · Physics 2025-09-12 Devanshi Arora

We demonstrate on the example of the dc+ac driven overdamped Frenkel-Kontorova model that an easily calculable measure of complexity can be used for the examination of Shapiro steps in presence of thermal noise. In real systems, thermal…

The determination of the absolute scale of the neutrino masses is one of the most challenging present questions in particle physics. The most stringent limit, $m(\bar{\nu}_{\mathrm{e}})<2$eV, was achieved for the electron anti-neutrino mass…

Semiconductor nanocrystals (quantum dots) are light emitters with high quantum yield that are relatively easy to manufacture. There is therefore much interest in their possible application for the development of high-performance…

Results obtained from an analysis of the energy spectrum of cosmic rays with energies in the region of $E_0 \ge 10^{17}$ eV over the period of continuous observations from 1974 to 2017 are presented. A refined expression for estimating the…

High Energy Astrophysical Phenomena · Physics 2023-01-25 A. V. Glushkov , M. I. Pravdin , A. V. Sabourov

We describe the electromagnetic calorimeter built for the GRAAL apparatus at the ESRF. Its monitoring system is presented in detail. Results from tests and the performance obtained during the first GRAAL experiments are given. The energy…

A silicon-tungsten (Si-W) sampling calorimeter, consisting of 19 alternate layers of silicon pad detectors (individual pad area of 1~cm$^2$) and tungsten absorbers (each of one radiation length), has been constructed for measurement of…

The NA64 experiment at CERN H4 beamline recently started a high-energy positron-beam program to search for light dark matter particles through a thick-target, missing-energy measurement. To fulfil the energy resolution requirement of the…

Instrumentation and Detectors · Physics 2026-03-24 Andrei Antonov , Pietro Bisio , Mariangela Bondì , Andrea Celentano , Anna Marini , Luca Marsicano

Responses of surface and underground scintillation detectors of Yakutsk array are calculated for showers initiated by primary particles with energy E0>=1.0E17 eV within the frameworks of QGSJet01 QGSIIJet-II-04, SIBYLL-2.1 and EPOS-LHC…

High Energy Astrophysical Phenomena · Physics 2015-06-22 A. V. Glushkov , M. I. Pravdin , A. Sabourov

We propose to measure the energy correlator in quarkonium production, which tracks the energy deposited in the calorimeter $\chi$-angular distance away from the identified quarkonium. The observable eliminates the need for jets while…

High Energy Physics - Phenomenology · Physics 2024-11-07 An-Ping Chen , Xiaohui Liu , Yan-Qing Ma

The MINERvA collaboration operated a scaled-down replica of the solid scintillator tracking and sampling calorimeter regions of the MINERvA detector in a hadron test beam at the Fermilab Test Beam Facility. This article reports measurements…

One of the most important requirements for a detector at the ILC is good jet energy resolution. It is widely believed that the particle flow approach to calorimetry is the key to achieving the goal of 0.3/sqrt(E[GeV]). This paper describes…

Instrumentation and Detectors · Physics 2008-11-07 M. A. Thomson

A prototype silicon-tungsten electromagnetic calorimeter for an ILC detector was tested in 2007 at the CERN SPS test beam. Data were collected with electron and hadron beams in the energy range 8 to 80 GeV. The analysis described here…

Instrumentation and Detectors · Physics 2014-11-20 C. Adloff , Y. Karyotakis , J. Repond , J. Yu , G. Eigen , Y. Mikami , N. K. Watson , J. A. Wilson , T. Goto , G. Mavromanolakis , M. A. Thomson , D. R. Ward , W. Yan , D. Benchekroun , A. Hoummada , Y. Khoulaki , J. Apostolakis , A. Ribon , V. Uzhinskiy , M. Benyamna , C. Cârloganu , F. Fehr , P. Gay , G. C. Blazey , D. Chakraborty , A. Dyshkant , K. Francis , D. Hedin , J. G. Lima , V. Zutshi , J. -Y. Hostachy , K. Krastev , L. Morin , N. D'Ascenzo , U. Cornett , D. David , R. Fabbri , G. Falley , K. Gadow , E. Garutti , P. Göttlicher , T. Jung , S. Karstensen , A. -I. Lucaci-Timoce , B. Lutz , N. Meyer , V. Morgunov , M. Reinecke , F. Sefkow , P. Smirnov , A. Vargas-Trevino , N. Wattimena , O. Wendt , N. Feege , M. Groll , J. Haller , R. -D. Heuer , S. Morozov , S. Richter , J. Samson , A. Kaplan , H. -Ch. Schultz-Coulon , W. Shen , A. Tadday , B. Bilki , E. Norbeck , Y. Onel , E. J. Kim , G. Kim , D-W. Kim , K. Lee , S. C. Lee , K. Kawagoe , Y. Tamura , P. D. Dauncey , A. -M. Magnan , H. Yilmaz , O. Zorba , V. Bartsch , M. Postranecky , M. Warren , M. Wing , M. G. Green , F. Salvatore , M. Bedjidian , R. Kieffer , I. Laktineh , M. -C. Fouz , D. S. Bailey , R. J. Barlow , M. Kelly , R. J. Thompson , M. Danilov , E. Tarkovsky , N. Baranova , D. Karmanov , M. Korolev , M. Merkin , A. Voronin , A. Frey , S. Lu , K. Seidel , F. Simon , C. Soldner , L. Weuste , J. Bonis , B. Bouquet , S. Callier , P. Cornebise , Ph. Doublet , M. Faucci Giannelli , J. Fleury , H. Li , G. Martin-Chassard , F. Richard , Ch. de la Taille , R. Poeschl , L. Raux , N. Seguin-Moreau , F. Wicek , M. Anduze , V. Boudry , J-C. Brient , G. Gaycken , D. Jeans , P. Mora de Freitas , G. Musat , M. Reinhard , A. Rougé , M. Ruan , J-Ch. Vanel , H. Videau , K-H. Park , J. Zacek , J. Cvach , P. Gallus , M. Havranek , M. Janata , M. Marcisovsky , I. Polak , J. Popule , L. Tomasek , M. Tomasek , P. Ruzicka , P. Sicho , J. Smolik , V. Vrba , J. Zalesak , B. Belhorma , M. Belmir , S. W. Nam , I. H. Park , J. Yang , Jong-Seo Chai , Jong-Tae Kim , Geun-Bum Kim , J. Kang , Y. -J. Kwon

An important experiment for cosmic ray physics is going to be conducted with the colliding proton beams of the CERN LHC. The equivalent energy of the 14 TeV center of mass energy of the colliding proton beams in the LHC is 1017eV in the…

High Energy Physics - Phenomenology · Physics 2008-11-26 O. Adriani

Data from KEK on subthreshold antiproton as well as on pi(+-) and K(+-) production in proton-nucleus reactions are described at projectile energies between 3.5 and 12.0 GeV. We use a model which considers a hadron-nucleus reaction as an…

Nuclear Theory · Physics 2008-11-26 V. I. Komarov , H. Mueller , A. Sibirtsev

The electromagnetic barrel calorimeter is one of the main components of the planned GlueX experiment. It will consist of 48 modules made of consecutive layers of 4 m long lead sheet and fast green scintillator fibers for an overall number…

Instrumentation and Detectors · Physics 2009-11-13 M. Barbi

Balloon- and space-borne cosmic-ray experiments employ plastic scintillators read out by silicon photomultipliers (SiPMs) to achieve picosecond-level time resolutions for triggering and particle identification. The performance of these…

Instrumentation and Detectors · Physics 2025-11-14 José Reyes Castillo , Saúl Aguilar Salazar , Diego Mauricio Gomez Coral

The electromagnetic calorimeter for the new muon (g-2) experiment at Fermilab will consist of arrays of PbF2 Cherenkov crystals read out by large-area silicon photo-multiplier (SiPM) sensors. We report here on measurements and simulations…

We present first experimental data on the high energy behavior of helium atoms quantum reflecting from the nanoscopically disordered surface of a quartz crystal. The use of the light, stable and inert He atom not only opens the unique…

Quantum Physics · Physics 2009-11-07 V. Druzhinina , M. DeKieviet
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