The CMS barrel calorimeter response to particle beams from 2 to 350 GeV/c

Abdullin, S.; Abramov, V.; Acharya, B. S.; Adam, N.; Adams, M. R.; Adžić, P.; Akchurin, N.; Akgun, U.; Albayrak, E. A.; Alemany–Fernández, R.; Almeida, N.; Anagnostou, G.; Andelin, D.; Anderson, E. W.; Anfreville, M.; Aničin, I.; Antchev, G.; Antunović, Ž.; Arcidiacono, R.; Arenton, M. W.; Auffray, E.; Argirò, S.; Askew, A.; Atramentov, O.; Ayan, S.; Arcidy, M.; Aydin, S.; Aziz, T.; Baarmand, M. M.; Babich, K.; Baccaro, S.; Baden, Drew; Baffioni, S.; Bakirci, Mustafa Numan; Balazs, M.; Banerjee, S.; Banerjee, S.; Bard, Robert L.; Barge, D.; Barnes, V. E.; Barney, D.; Barone, L.; Bartoloni, Alessandro; Baty, C.; Bawa, H. S.; Baiatian, G.; Bandurin, D. V.; Beauceron, S.; Bell, K. W.; Bencze, G.; Benetta, R.; Bercher, M.; Beri, S. B.; Bernet, C.; Berntzon, L.; Berthon, U.; Besançon, M.; Betev, B. L.; Beuselinck, R.; Bhatnagar, V.; Bhatti, A.; Biino, C.; Blaha, J.; Bloch, P.; Blyth, S.; Bodek, A.; Bornheim, A.; Böse, S.; Bose, T.; Bourotte, J.; Brett, A. M.; Brown, R. M.; Britton, D.; Budd, H. S.; Buehler, M.; Burchesky, K.; Busson, P.; Camanzi, B.; Camporesi, T.; Cankoçak, K.; Carrell, K.; Carrera, E.; Cartiglia, N.; Cavallari, F.; Çerçi, S.; Cerutti, M.; Chang, P.; Chang, Y. H.; Charlot, C.; Chen, E. A.; Chen, W. T.; Chen, Z.; Chendvankar, S. R.; Chipaux, R.; Choudhary, B. C.; Choudhury, R. K.; Chung, Y. S.; Clarida, W.; Cockerill, D. J. A.; Combaret, C.; Conetti, S.; Cossutti, F.; Cox, B. E.; Cremaldi, L.; Cushman, P.; Cussans, D.; Dafinei, I.; Damgov, J.; Calafiori, D. R. Da Silva Di; Daskalakis, G.; Davatz, G.; David, A.; Barbaro, P. de; Debbins, P.; Deiters, K.; Déjardin, M.; Djordjevic, M.; Deliomeroglu, M.; Negra, R. Della; Ricca, G. Della; Re, D. Del; Demianov, A. I.; Min, A. De; Denegri, D.; Depasse, P.; Visser, T. De; Descamps, J.; Deshpande, P. V.; Diaz, J. C.; Diemoz, M.; Marco, E. Di; Дімітров, Л.; Dissertori, G.; Dittmar, M.; Djambazov, L.; Dobrzyński, L.; Drndarevic, S.; Duboscq, J. 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M.; Silva, J.; Silva, P.; Skuja, A.; Sharma, S.; Sherwood, B.; Shiu, J. G.; Shivpuri, R. K.; Shukla, P.; Shumeiko, N.; Смирнов, В. И.; Smith, Brett; Smith, V. J.; Sogut, K.; Sönmez, N.; Sorokin, P.; Spezziga, M.; Sproston, M.; Stefanovich, R.; Stöckli, F.; Stolin, V.; Sudhakar, K.; Sulak, L.; Suter, H.; Suzuki, I.; Swain, J.; Fatis, T. Tabarelli de; Talov, V. V.; Takahashi, Masashi; Tcheremoukhine, A.; Teller, O.; Teplov, K.; Theofilatos, K.; Thiebaux, Ch; Thomas, R.; Timciuc, V.; Timlin, C.; Titov, M.; Tobías, Aurelio; Tonwar, S. C.; Topakli, H.; Topkar, A.; Triantis, F. A.; Troshin, S.; Tully, C.; Turchanovich, L.K.; Tyurin, N.; Ueno, K.; Ulyanov, A.; Uzunian, A.; Vanini, A.; Vankov, I.; Vardanyan, I.; Varela, Fernando; Varela, José Arana; Vasil’ev, A. N.; Velasco, M.; Vergili, M.; Verma, Piyush; Verrecchia, P.; Vesztergombi, G.; Veverka, J.; Vichoudis, P.; Vidal, R.; Virdee, T.; Vishnevskiy, A.; Vlassov, E.; Vodopiyanov, I.; Volobouev, I.; Volkov, Alexey; Volodko, A.; Gunten, H. P. Von; Wang, L.; Wang, M.; Wardrope, D. R.; Weber, Martin; Weng, J.; Werner, J. S.; Wetstein, M.; Winn, D.; Wigmans, R.; Williams, J. H.; Whitmore, J.; Won, S.; Wu, S.; Yang, Y.; Yaselli, I.; Yazgan, E.; Yetkin, T.; Yohay, R.; Zabi, A.; Zalán, P.; Zamiatin, N.; Zarubin, A.; Zelepoukine, S.; Zeyrek, M.; Zhang, J.; Zhang, L. Y.; Zhu, K.; Zhu, R. Y.

doi:10.1140/epjc/s10052-009-1024-0

Cited by 10 publications

(6 citation statements)

References 4 publications

(4 reference statements)

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“…The energy scale in data agrees with that in the simulation to better than 1 (3)% in the barrel (endcap) region, |η| < 1.5 (1.3 < |η| < 3.0) [37]. Hadron calorimeter cells in the |η| < 3 region are calibrated primarily with test beam data and radioactive sources [38,39]. A more…”

Section: Cms Detectorsupporting

confidence: 53%

Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV

Khachatryan¹,

Erbacher²,

Montoya³

et al. 2016

J. High Energ. Phys.

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An analysis of dijet events in PbPb and pp collisions is performed to explore the properties of energy loss by partons traveling in a quark-gluon plasma. Data are collected at a nucleon-nucleon center-of-mass energy of 2.76 TeV at the LHC. The distribution of transverse momentum (p T ) surrounding dijet systems is measured by selecting charged particles in different ranges of p T and at different angular cones of pseudorapidity and azimuth. The measurement is performed as a function of centrality of the PbPb collisions, the p T asymmetry of the jets in the dijet pair, and the distance parameter R used in the anti-k T jet clustering algorithm. In events with unbalanced dijets, PbPb collisions show an enhanced multiplicity in the hemisphere of the subleading jet, with the p T imbalance compensated by an excess of low-p T particles at large angles from the jet axes.

show abstract

Section: Cms Detectorsupporting

confidence: 53%

Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV

Khachatryan¹,

Erbacher²,

Montoya³

et al. 2016

J. High Energ. Phys.

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“…Hadron calorimeter cells in the |η| < 3 region are calibrated primarily with test-beam data and radioactive sources [19,20]. A detailed description of the CMS detector may be found in [21].…”

Section: Jhep06(2012)160mentioning

confidence: 99%

Shape, transverse size, and charged-hadron multiplicity of jets in pp collisions at $ \sqrt{s}=7\;TeV $

Chatrchyan¹,

Khachatryan²,

Sirunyan³

et al. 2012

J. High Energ. Phys.

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Shape, transverse size, and charged-hadron multiplicity of jets in pp collisions at √ s = 7 TeVThe CMS collaboration Abstract: Measurements of jet characteristics from inclusive jet production in protonproton collisions at a centre-of-mass energy of 7 TeV are presented. The data sample was collected with the CMS detector at the LHC during 2010 and corresponds to an integrated luminosity of 36 pb −1 . The mean charged-hadron multiplicity, the differential and integral jet shape distributions, and two independent moments of the shape distributions are measured as functions of the jet transverse momentum for jets reconstructed with the anti-k T algorithm. The measured observables are corrected to the particle level and compared with predictions from various QCD Monte Carlo generators.

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“…than the π ± one in the CMS result [15]. In the same paper results concerning the response of charged kaons and antiprotons for momenta below 9 GeV/c are reported.…”

Section: Comparison Between Pion Kaon and Proton Energy Responses And Resolutionsmentioning

confidence: 74%

Study of energy response and resolution of the ATLAS Tile Calorimeter to hadrons of energies from 16 to 30 GeV

Abdallah¹,

Angelidakis²,

Arabidze³

et al. 2021

Eur. Phys. J. C

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Three spare modules of the ATLAS Tile Calorimeter were exposed to test beams from the Super Proton Synchrotron accelerator at CERN in 2017. The detector’s measurements of the energy response and resolution to positive pions and kaons, and protons with energies ranging from 16 to 30 GeV are reported. The results have uncertainties of a few percent. They were compared to the predictions of the Geant4-based simulation program used in ATLAS to estimate the response of the detector to proton-proton events at the Large Hadron Collider. The determinations obtained using experimental and simulated data agree within the uncertainties.

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The CMS barrel calorimeter response to particle beams from 2 to 350 GeV/c

Cited by 10 publications

References 4 publications

Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV

Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at s N N = 2.76 $$ \sqrt{s_{\mathrm{NN}}}=2.76 $$ TeV

Shape, transverse size, and charged-hadron multiplicity of jets in pp collisions at $ \sqrt{s}=7\;TeV $

Study of energy response and resolution of the ATLAS Tile Calorimeter to hadrons of energies from 16 to 30 GeV

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