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Related papers: The CASTOR calorimeter at the CMS experiment

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The HL-LHC will challenge the detectors with a nearly 10-fold increase in integrated luminosity compared to the previous LHC runs combined, thus the CMS detector will be upgraded to face the higher levels of radiation and the larger amounts…

Instrumentation and Detectors · Physics 2026-03-10 CMS HGCAL collaboration

A prototype Silicon-Tungsten electromagnetic calorimeter (ECAL) for an International Linear Collider (ILC) detector was installed and tested during summer and autumn 2006 at CERN. The detector had 6480 silicon pads of dimension 1x1 cm^2.…

Instrumentation and Detectors · Physics 2017-07-24 CALICE Collaboration

A Lead Tungstate crystal produced for the electromagnetic calorimeter of the CMS experiment at the LHC was cut into three equal-length sections. The central one was irradiated with 290 MeV/c positive pions up to a fluence of (5.67 +-…

Instrumentation and Detectors · Physics 2009-11-13 P. Lecomte , D. Luckey , F. Nessi-Tedaldi , F. Pauss , D. Renker

A simple and low cost apparatus has been designed and built to measure the electrical resistivity, ($\rho$), of metal and semiconductors in 300-620 K temperature range. The present design is suitable to do measurement on rectangular bar…

General Physics · Physics 2017-04-14 Saurabh Singh , Sudhir K. Pandey

The PADME experiment, hosted at the Laboratori Nazionali di Frascati in Italy, is dedicated to the dark photon search. It looks for the reaction $e^{+}\,e^{-}\rightarrow A'\,\gamma$, where $A'$ indicates the dark photon. The…

Instrumentation and Detectors · Physics 2020-06-17 Gabriele Piperno

The CALICE Semi-Digital Hadron Calorimeter (SDHCAL) technological prototype is a sampling calorimeter using Glass Resistive Plate Chamber detectors with a three-threshold readout as the active medium. This technology is one of the two…

Instrumentation and Detectors · Physics 2016-07-13 Z. Deng , Y. Li , Y. Wang , Q. Yue , Z. Yang , J. Apostolakis , G. Folger , C. Grefe , V. Ivantchenko , A. Ribon , V. Uzhinskiy , D. Boumediene , C. Carloganu , V. Français , G. Cho , D-W. Kim , S. C. Lee , W. Park , S. Vallecorsa , S. Cauwenbergh , M. Tytgat , A. Pingault , N. Zaganidis , E. Brianne , A. Ebrahimi , K. Gadow , P. Göttlicher , C. Günter , O. Hartbrich , B. Hermberg , A. Irles , F. Krivan , K. Krüger , J. Kvasnicka , S. Lu , B. Lutz , V. Morgunov , C. Neubüser , A. Provenza , M. Reinecke , F. Sefkow , S. Schuwalow , H. L. Tran , E. Garutti , S. Laurien , M. Matysek , M. Ramilli , S. Schroeder , B. Bilki , E. Norbeck , D. Northacker , Y. Onel , S. Chang , A. Khan , D. H. Kim , D. J. Kong , Y. D. Oh , K. Kawagoe , H. Hirai , Y. Sudo , T. Suehara , H. Sumida , T. Yoshioka , E. Cortina Gil , S. Mannai , V. Buridon , C. Combaret , L. Caponetto , R. Eté , G. Garillot , 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 , M. Chadeeva , M. Danilov , M. Gabriel , P. Goecke , C. Kiesling , N. vanderKolk , F. Simon , M. Szalay , S. Bilokin , J. Bonis , P. Cornebise , F. Richard , R. Pöschl , J. Rouëné , A. Thiebault , D. Zerwas , M. Anduze , V. Balagura , K. Belkadhi , V. Boudry , J-C. Brient , R. Cornat , M. Frotin , F. Gastaldi , Y. Haddad , F. Magniette , M. Ruan , M. Rubio-Roy , K. Shpak , H. Videau , D. Yu , S. Callier , S. Conforti di Lorenzo , F. Dulucq , G. Martin-Chassard , Ch. de la Taille , L. Raux , N. Seguin-Moreau , K. Kotera , H. Ono , T. Takeshita , F. Corriveau

Very Large Area gamma-ray Space Telescope (VLAST) is the next-generation flagship space observatory for high-energy gamma-ray detection proposed by China. The observation energy range covers from MeV to TeV and beyond, with acceptance of 10…

Measuring the depth of interaction in thick Cadmium-Zinc-Telluride (CZT) detectors allows improved imaging and spectroscopy for hard X-ray imaging above 100 keV. The Energetic X-ray Imaging Survey Telescope (EXIST) will employ relatively…

Astrophysics · Physics 2009-11-10 J. Hong , E. C. Bellm , J. E. Grindlay , T. Narita

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…

With an active silicon area of more than 200 squaremetres, the silicon strip tracker of the CMS experiment, one of the experiments currently under construction for the future Large Hadron Collider at CERN, will be by far the largest silicon…

Instrumentation and Detectors · Physics 2008-11-26 Katja Klein

The CMS hadron Calorimeter is made of alternating layers of scintillating tiles and metals, such as brass or iron. The original photo detectors were hybrid units with a single accelerating gap called Hybrid Photo Diodes (HPD). Scintillating…

Instrumentation and Detectors · Physics 2018-06-27 R A Shukla , V G Achanta , P D Barbaro , S R Dugad , A Heering , S K Gupta , I Mirza , S S Prabhu , P Rumerio

The Phase-1 upgrade of the CMS pixel detector is built out of four barrel layers (BPix) and three forward disks in each endcap (FPix). It comprises a total of 124M pixel channels in 1,856 modules, and it is designed to withstand…

Instrumentation and Detectors · Physics 2017-10-02 Weinan Si

Hadronic reactions producing strange quarks such as exclusive or semi-inclusive kaon production, play an important role in studies of hadron structure and the dynamics that bind the most basic elements of nuclear physics. The small-angle…

Microcalorimeter instruments aboard future X-ray observatories will require an anti-coincidence (anti-co) detector to veto charged particle events and reduce the non-X-ray background. We have developed a large-format, TES-based prototype…

A differential, membrane-based nanocalorimeter for general specific heat studies of very small samples, ranging from 0.5 mg to sub-{\mu}g in mass, is described. The calorimeter operates over the temperature range from above room temperature…

Instrumentation and Detectors · Physics 2012-08-20 S. Tagliati , V. M. Krasnov , A. Rydh

The Particle Flow Algorithms adopted for future $e^{+}e^{-}$ colliders detectors and phase-II CMS upgrade require very high granularity calorimeters to deconvolve the individual contributions of particles in jets. This is especially true…

Instrumentation and Detectors · Physics 2017-11-27 Kostiantyn Shpak

To define the work performed on a driven quantum system in a physically sound way has turned out to be a truly non-trivial task, except in some special cases of limited applicability. This topic has been in a focus of intense research…

Statistical Mechanics · Physics 2012-12-27 Jukka P. Pekola , Paolo Solinas , Alexander Shnirman , Dmitri V. Averin

Quartz fiber calorimetry is a technique the signal generation mechanism of which is based on the Cherenkov effect. In this article we try to give a comprehensive overview of the subject. We start with a general introduction to calorimetry…

Instrumentation and Detectors · Physics 2007-05-23 G. Mavromanolakis

The Resistive Plate Chambers (RPCs) are employed in the CMS experiment at the LHC as dedicated trigger system both in the barrel and in the endcap. This note presents results of the RPC detector uniformity and stability during the 2011 data…

We discuss a CMS eXtension for Studying Energetic Neutrinos (CMS-XSEN). Neutrinos at the LHC are abundant and have unique features: their energies reach out to the TeV range, and the contribution of the {\tau} flavour is sizeable. The…

Instrumentation and Detectors · Physics 2018-04-13 S. Buontempo , G. M. Dallavalle , G. De Lellis , D. Lazic , F. L. Navarria