000490329 001__ 490329
000490329 005__ 20231224023219.0
000490329 0247_ $$2INSPIRETeX$$aCMS:2022qan
000490329 0247_ $$2inspire$$ainspire:2178613
000490329 0247_ $$2arXiv$$aarXiv:2211.04740
000490329 0247_ $$2datacite_doi$$a10.3204/PUBDB-2022-07658
000490329 037__ $$aPUBDB-2022-07658
000490329 041__ $$aEnglish
000490329 088__ $$2arXiv$$aarXiv:2211.04740
000490329 1001_ $$0P:(DE-HGF)0$$aCMS Collaboration$$b0$$eCollaboration author
000490329 245__ $$aPerformance of the CMS High Granularity Calorimeter prototype to charged pion beams of 20$-$300 GeV/c
000490329 260__ $$c2022
000490329 3367_ $$0PUB:(DE-HGF)25$$2PUB:(DE-HGF)$$aPreprint$$bpreprint$$mpreprint$$s1674475315_20778
000490329 3367_ $$2ORCID$$aWORKING_PAPER
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000490329 3367_ $$2BibTeX$$aARTICLE
000490329 3367_ $$2DataCite$$aOutput Types/Working Paper
000490329 500__ $$aSubmitted to JINST
000490329 520__ $$aThe upgrade of the CMS experiment for the high luminosity operation of the LHC comprises the replacement of the current endcap calorimeter by a high granularity sampling calorimeter (HGCAL). The electromagnetic section of the HGCAL is based on silicon sensors interspersed between lead and copper (or copper tungsten) absorbers. The hadronic section uses layers of stainless steel as an absorbing medium and silicon sensors as an active medium in the regions of high radiation exposure, and scintillator tiles directly readout by silicon photomultipliers in the remaining regions. As part of the development of the detector and its readout electronic components, a section of a silicon-based HGCAL prototype detector along with a section of the CALICE AHCAL prototype was exposed to muons, electrons and charged pions in beam test experiments at the H2 beamline at the CERN SPS in October 2018. The AHCAL uses the same technology as foreseen for the HGCAL but with much finer longitudinal segmentation. The performance of the calorimeters in terms of energy response and resolution, longitudinal and transverse shower profiles is studied using negatively charged pions, and is compared to GEANT4 predictions. This is the first report summarizing results of hadronic showers measured by the HGCAL prototype using beam test data.
000490329 536__ $$0G:(DE-HGF)POF4-611$$a611 - Fundamental Particles and Forces (POF4-611)$$cPOF4-611$$fPOF IV$$x0
000490329 536__ $$0G:(EU-Grant)654168$$aAIDA-2020 - Advanced European Infrastructures for Detectors at Accelerators (654168)$$c654168$$fH2020-INFRAIA-2014-2015$$x1
000490329 588__ $$aDataset connected to INSPIRE
000490329 650_7 $$2INSPIRE$$api: irradiation
000490329 650_7 $$2INSPIRE$$amuon: irradiation
000490329 650_7 $$2INSPIRE$$aelectron: irradiation
000490329 650_7 $$2INSPIRE$$acalorimeter: performance
000490329 650_7 $$2INSPIRE$$acalorimeter: hadronic
000490329 650_7 $$2INSPIRE$$acalorimeter: electromagnetic
000490329 650_7 $$2INSPIRE$$aCMS
000490329 650_7 $$2INSPIRE$$ashowers: spatial distribution
000490329 650_7 $$2INSPIRE$$aelectronics: readout
000490329 650_7 $$2INSPIRE$$anumerical calculations
000490329 650_7 $$2INSPIRE$$aGEANT
000490329 650_7 $$2INSPIRE$$aresolution
000490329 650_7 $$2INSPIRE$$aCALICE
000490329 693__ $$0EXP:(DE-H253)LHC-Exp-CMS-20150101$$1EXP:(DE-588)4398783-7$$5EXP:(DE-H253)LHC-Exp-CMS-20150101$$aLHC$$eLHC: CMS$$x0
000490329 7001_ $$0P:(DE-HGF)0$$aCALICE Collaboration$$b1$$eCollaboration Author
000490329 8564_ $$uhttps://arxiv.org/abs/2211.04740
000490329 8564_ $$uhttps://bib-pubdb1.desy.de/record/490329/files/2211.04740.pdf$$yOpenAccess
000490329 8564_ $$uhttps://bib-pubdb1.desy.de/record/490329/files/2211.04740.pdf?subformat=pdfa$$xpdfa$$yOpenAccess
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000490329 9131_ $$0G:(DE-HGF)POF4-611$$1G:(DE-HGF)POF4-610$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMatter and the Universe$$vFundamental Particles and Forces$$x0
000490329 9141_ $$y2022
000490329 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000490329 915__ $$0LIC:(DE-HGF)CCBYNCND4$$2HGFVOC$$aCreative Commons Attribution-NonCommercial-NoDerivs CC BY-NC-ND 4.0
000490329 915__ $$0StatID:(DE-HGF)0580$$2StatID$$aPublished
000490329 9201_ $$0I:(DE-H253)FTX-20210408$$kFTX$$lTechnol. zukünft. Teilchenph. Experim.$$x0
000490329 9201_ $$0I:(DE-H253)CMS-20120731$$kCMS$$lLHC/CMS Experiment$$x1
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000490329 980__ $$aI:(DE-H253)FTX-20210408
000490329 980__ $$aI:(DE-H253)CMS-20120731
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