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The long slab is a new prototype for the SiW-Ecal, a silicon tungsten electromagnetic calorimeter for the ILD detector of the future International Linear Collider. This new prototype has been designed to demonstrate the ability to build a…

An analog hadron calorimeter (AHCAL) prototype of 5.3 nuclear interaction lengths thickness has been constructed by members of the CALICE Collaboration. The AHCAL prototype consists of a 38-layer sandwich structure of steel plates and…

Instrumentation and Detectors · Physics 2016-12-13 C. Adloff , Y. Karyotakis , J. Repond , A. Brandt , H. Brown , K. De , C. Medina , J. Smith , J. Li , M. Sosebee , A. White , J. Yu , T. Buanes , G. Eigen , Y. Mikami , O. Miller , N. K. Watson , J. A. Wilson , T. Goto , G. Mavromanolakis , M. A. Thomson , D. R. Ward , W. Yan , D. Benchekroun , A. Hoummada , Y. Khoulaki , M. Oreglia , M. Benyamna , C. Cârloganu , P. Gay , J. Ha , G. C. Blazey , D. Chakraborty , A. Dyshkant , K. Francis , D. Hedin , G. Lima , V. Zutshi , V. A. Babkin , S. N. Bazylev , Yu. I. Fedotov , V. M. Slepnev , I. A. Tiapkin , S. V. Volgin , J. -Y. Hostachy , L. Morin , N. D?Ascenzo , U. Cornett , D. David , R. Fabbri , G. Falley , N. Feege , K. Gadow , E. Garutti , P. Göttlicher , T. Jung , S. Karstensen , V. Korbel , A. -I. Lucaci-Timoce , B. Lutz , N. Meyer , V. Morgunov , M. Reinecke , S. Schätzel , S. Schmidt , F. Sefkow , P. Smirnov , A. Vargas-Trevino , N. Wattimena , O. Wendt , M. Groll , R. -D. Heuer , 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 , J. A. Ballin , P. D. Dauncey , A. -M. Magnan , H. Yilmaz , O. Zorba , V. Bartsch , M. Postranecky , M. Warren , M. Wing , M. Faucci Giannelli , M. G. Green , F. Salvatore , R. Kieffer , I. Laktineh , M. C Fouz , D. S. Bailey , R. J. Barlow , R. J. Thompson , M. Batouritski , O. Dvornikov , Yu. Shulhevich , N. Shumeiko , A. Solin , P. Starovoitov , V. Tchekhovski , A. Terletski , B. Bobchenko , M. Chadeeva , M. Danilov , O. Markin , R. Mizuk , V. Morgunov , E. Novikov , V. Rusinov , E. Tarkovsky , V. Andreev , N. Kirikova , A. Komar , V. Kozlov , P. Smirnov , Y. Soloviev , A. Terkulov , P. Buzhan , B. Dolgoshein , A. Ilyin , V. Kantserov , V. Kaplin , A. Karakash , E. Popova , S. Smirnov , N. Baranova , E. Boos , L. Gladilin , D. Karmanov , M. Korolev , M. Merkin , A. Savin , A. Voronin , A. Topkar , A. Freyk , C. Kiesling , S. Lu , K. Prothmann , K. Seidel , F. Simon , C. Soldner , L. Weuste , B. Bouquet , S. Callier , P. Cornebise , F. Dulucq , J. Fleury , H. Li , G. Martin-Chassard , F. Richard , Ch. de la Taille , R. Poeschl , L. Raux , M. Ruan , N. Seguin-Moreau , F. Wicek , M. Anduze , V. Boudry , J-C. Brient , G. Gaycken , R. Cornat , D. Jeans , P. Mora de Freitas , G. Musat , M. Reinhard , A. Rougé , J-Ch. Vanel , H. Videau , K-H. Park , J. Zacek , J. Cvach , P. Gallus , M. Havranek , M. Janata , J. Kvasnicka , M. Marcisovsky , I. Polak , J. Popule , L. Tomasek , M. Tomasek , P. Ruzicka , P. Sicho , J. Smolik , V. Vrba , J. Zalesak , Yu. Arestov , V. Ammosov , B. Chuiko , V. Gapienko , Y. Gilitski , V. Koreshev , A. Semak , Yu. Sviridov , V. Zaets , B. Belhorma , M. Belmir , A. Baird , R. N. Halsall , S. W. Nam , I. H. Park , J. Yang , Jong-Seo Chai , Jong-Tae Kim , Geun-Bum Kim , Y. Kim , J. Kang , Y. -J. Kwon , Ilgoo Kim , Taeyun Lee , Jaehong Park , Jinho Sung , S. Itoh , K. Kotera , M. Nishiyama , T. Takeshita , S. Weber , C. Zeitnitz

The CALICE Semi-Digital Hadron Calorimeter technological prototype completed in 2011 is a sampling calorimeter using Glass Resistive Plate Chamber (GRPC) detectors as the active medium. This technology is one of the two options proposed for…

The next generation of bolometric experiments searching for rave events, in particular for the neutrino-less double beta decay, needs fast, high-sensitivity and easy-to-scale cryogenic light detectors. The CALDER project (2014-2020)…

The low-x gluon density in the proton and, in particular, in nuclei is only very poorly constrained, while a better understanding of the low-x structure is crucial for measurements at the LHC and also for the planning of experiments at…

High Energy Physics - Experiment · Physics 2018-12-21 Thomas Peitzmann

The AMoRE collaboration searches for neutrinoless double beta decay of $^{100}$Mo using molybdate scintillating crystals via low temperature thermal calorimetric detection. The early phases of the experiment, AMoRE-pilot and AMoRE-I, have…

The first technological SDHCAL prototype having been successfully tested, a new phase of R&D, to validate completely the SDHCAL option for the International Linear Detector (ILD) project of the International Linear Collider (ILC), has…

Instrumentation and Detectors · Physics 2016-08-24 Antoine Pingault

CLIC is a proposed linear $e^{+}e^{-}$ collider with center-of-mass energies of up to $3\,\textrm{TeV}$. Its main objectives are precise top quark and Higgs boson measurements, as well as searches for Beyond Standard Model physics. To meet…

Instrumentation and Detectors · Physics 2018-12-07 Simon Spannagel

This note discusses methods of particle reconstruction in the forward region detectors of future e+e- linear colliders such as ILC or CLIC. At the nominal luminosity the innermost electromagnetic calorimeters undergo high particle fluxes…

Instrumentation and Detectors · Physics 2017-02-24 Andre Sailer , Andrey Sapronov

The Large Hadron Collider's high luminosity era presents major computational challenges in the analysis of collision events. Large amounts of Monte Carlo (MC) simulation will be required to constrain the statistical uncertainties of the…

The production of direct photons, not coming from hadron decays, at large transverse momentum pT > 2 GeV/c in proton-proton collisions at the LHC, is an interesting process to test the predictions of perturbative Quantum Chromodynamics at…

High Energy Physics - Experiment · Physics 2015-03-17 Raphaelle Ichou

The electromagnetic calorimeter (ECAL) of the AMS-02 experiment is a 3-dimensional sampling calorimeter, made of lead and scintillating fibers. The detector allows for a high granularity, with 18 samplings in the longitudinal direction, and…

The Future Circular Collider (FCC) is a post-LHC project aiming at searches for physics beyond the SM in a new 80--100~km tunnel at CERN. Running in its first phase as a very-high-luminosity electron-positron collider (FCC-ee), it will…

High Energy Physics - Phenomenology · Physics 2016-10-21 Peter Skands , David d'Enterria

This manuscript is devoted to the description of the proposed Future Circular Collider (FCC) project and its physics program focused on measurements involving heavy quarks. It summarizes the report submitted to the US 2021 Snowmass Process…

High Energy Physics - Experiment · Physics 2022-07-12 Radek Novotny

The motivation for PF calorimetry is to experimentally measure the energy of hadron jets with excellent resolution. In particle flow designs, sigma(E)/E < 5% should be possible for a range of jet energies from 50 GeV to 250 GeV, important…

Instrumentation and Detectors · Physics 2022-07-20 Randal Ruchti , Katja Kruger

A first prototype of a scintillator strip-based electromagnetic calorimeter was built, consisting of 26 layers of tungsten absorber plates interleaved with planes of 45x10x3 mm3 plastic scintillator strips. Data were collected using a…

Instrumentation and Detectors · Physics 2014-07-24 CALICE Collaboration , K. Francis , J. Repond , J. Schlereth , J. Smith , L. Xia , E. Baldolemar , J. Li , S. T. Park , M. Sosebee , A. P. White , J. Yu , G. Eigen , Y. Mikami , N. K. Watson , M. A. Thomson , D. R. Ward , D. Benchekroun , A. Hoummada , Y. Khoulaki , J. Apostolakis , A. Dotti , G. Folger , V. Ivantchenko , A. Ribon , 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 , K. Gadow , P. Goettlicher , C. Guenter , O. Hartbrich , B. Hermberg , S. Karstensen , F. Krivan , K. Krueger , B. Lutz , S. Morozov , V. Morgunov , C. Neubueser , M. Reinecke , F. Sefkow , P. Smirnov , M. Terwort , E. Garutti , S. Laurien , S. Lu , 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 , D. Besson , P. Buzhan , A. Ilyin , V. Kantserov , V. Kaplin , A. Karakash , E. Popova , V. Tikhomirov , C. Kiesling , K. Seidel , F. Simon , C. Soldner , 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 , H. Ono , T. Takeshita , S. Uozumi , D. Jeans , S. Chang , A. Khan , D. H. Kim , D. J. Kong , Y. D. Oh , M. Goetze , J. Sauer , S. Weber , C. Zeitnitz

In order to measure integrated luminosity with a required precision of $10^{-4}$ at the $Z^0$ pole, proposed CEPC $e^{+}e^{-}$ collider requires a luminometer, a specially designed calorimeter placed in the very forward region to identify…

High Energy Physics - Experiment · Physics 2024-07-04 Ivan Smiljanic , Ivanka Bozovic , Goran Kacarevic

A strong candidate for the Standard Model Scalar boson, H(126), has been discovered by the Large Hadron Collider (LHC) experiments. In order to study this fundamental particle with unprecedented precision, and to perform precision tests of…

The CALICE collaboration has constructed highly granular electromagnetic and hadronic calorimeter prototypes to evaluate technologies for the use in detector systems at a future Linear Collider. The hadron calorimeter uses small…

Instrumentation and Detectors · Physics 2019-08-13 Frank Simon

Diffuse X-ray Explorer (DIXE) is a proposed X-ray spectroscopic survey experiment for the China Space Station. Its detector assembly (DA) contains the transition edge sensor (TES) microcalorimeter and readout electronics based on the…

Instrumentation and Methods for Astrophysics · Physics 2024-05-14 Jiejia Liu , Sifan Wang , Hai Jin , Qian Wang , Wei Cui
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