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Polina Simkina
The Compact Muon Solenoid (CMS) is one of the general purpose detectors at the CERN Large Hadron Collider (LHC), where the products of proton?proton collisions at the center of mass energy up to 13.6 TeV are reconstructed. The electromagnetic calorimeter...
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Ziyu Zhang, Guang Zhao, Shengsen Sun, Qing Pu, Chunxiu Liu, Chunxu Yu, Dong Liu, Hang Qi, Guangshun Huang, Tobias Stockmanns, Beijiang Liu, Fei Wang, Yitong Zhang and Xiaoyan Shen
For high-energy π0" role="presentation">??0p0
p
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mesons, the angle between the two final-state photons decreases with the increase in the energy of the π0" role="presentation">??0p0
p
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, which enhances the probability of overlappin...
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Nural Akchurin, Christopher Cowden, Jordan Damgov, Adil Hussain and Shuichi Kunori
We report a greater than factor of two improvement in the hadronic energy resolution of a simulated Cherenkov calorimeter by estimating the energy with machine learning over traditional techniques. The prompt signal formation and energy threshold propert...
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Kalina Dimitrova and on behalf of the PADME collaboration
The PADME apparatus was built at the Frascati National Laboratory of INFN to search for a dark photon (A′" role="presentation">??'A'
A
'
) produced via the process e+e−→A′γ" role="presentation">??+??-...
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Sanghyun Ko, Hwidong Yoo and Seungkyu Ha
The dual-readout calorimeter has two channels, Cherenkov and scintillation, that measure the fraction of an electromagnetic (EM) component within a shower by using different responses of each channel to the EM and hadronic component. It can measure the e...
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Gabriele Bigongiari, Oscar Adriani, Giovanni Ambrosi, Philipp Azzarello, Andrea Basti, Eugenio Berti, Bruna Bertucci, Lorenzo Bonechi, Massimo Bongi, Sergio Bottai, Mirko Brianzi, Paolo Brogi, Guido Castellini, Enrico Catanzani, Caterina Checchia, Raffaello D?Alessandro, Sebastiano Detti, Matteo Duranti, Noemi Finetti, Valerio Formato, Maria Ionica, Paolo Maestro, Fernando Maletta, Pier Simone Marrocchesi, Nicola Mori, Lorenzo Pacini, Paolo Papini, Sergio Bruno Ricciarini, Gianluigi Silvestre, Piero Spillantini, Oleksandr Starodubtsev, Francesco Stolzi, Jung Eun Suh, Arta Sulaj, Alessio Tiberio and Elena VannucciniaddShow full author listremoveHide full author list
A space-based detector dedicated to measurements of γ" role="presentation">???
?
-rays and charged particles has to achieve a balance between different instrumental requirements. A good angular resolution is necessary for the γ" role=...
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Tomas Davidek
The Tile Calorimeter (TileCal) is the central hadronic calorimeter of the ATLAS experiment at the LHC. This sampling device is made of steel plates acting as absorber and scintillating tiles as active medium. The wavelength-shifting fibers collect the li...
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Nikolay Atanov, Vladimir Baranov, Leo Borrel, Caterina Bloise, Julian Budagov, Sergio Ceravolo, Franco Cervelli, Francesco Colao, Marco Cordelli, Giovanni Corradi, Yuri Davydov, Stefano Di Falco, Eleonora Diociaiuti, Simone Donati, Bertrand Echenard, Carlo Ferrari, Antonio Gioiosa, Simona Giovannella, Valerio Giusti, Vladimir Glagolev, Francesco Grancagnolo, Dariush Hampai, Fabio Happacher, David Hitlin, Matteo Martini, Sophie Middleton, Stefano Miscetti, Luca Morescalchi, Daniele Paesani, Daniele Pasciuto, Elena Pedreschi, Frank Porter, Fabrizio Raffaelli, Alessandro Saputi, Ivano Sarra, Franco Spinella, Alessandra Taffara, Anna Maria Zanetti and Ren Yuan ZhuaddShow full author listremoveHide full author list
The Mu2e experiment at Fermilab will search for the standard model-forbidden, charged lepton flavour-violating conversion of a negative muon into an electron in the field of an aluminium nucleus. The distinctive signal signature is represented by a mono-...
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Louis Portalès
The CMS collaboration is building a high-granularity calorimeter (HGCAL) for the endcap regions as part of its planned upgrade for the High-Luminosity LHC. The calorimetric data will form part of the Level-1 trigger (hardware) of the CMS experiment, redu...
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Radoslav Simeonov
The forward calorimeter (FoCal) of ALICE, planned to be operational for LHC Run 4, will cover the pseudorapidity range 3.4 ≤η≤" role="presentation" style="position: relative;">=??==?=
=
?
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5.8 allowing to probe the unexp...
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