Results from a combined test of an electromagnetic liquid argon calorimeter with a hadronic scintillating-tile calorimeter

Ajaltouni, Z.; Albiol, F.; Алифанов, А. В.; Amaral, P.; Ambrosini, G.; Amorim, A.; Anderson, K. J.; Astvatsaturov, A.; Aubert, B.; Augé, E.; Autiero, D.; Azuelos, G.; Badaud, F.; Baisin, L.; Battistoni, G.; Bazan, A.; Bee, C. P.; Bellettini, G.; Berglund, S.; Berset, J.C.; Blaj, C.; Blanchot, G.; Blucher, E.; Bogush, A.A.; Böhm, C.; Boldea, V.; Borisov, O. N.; Bosman, M.; Bouhemaid, N.; Brette, P.; Bromberg, C.; Brossard, Michel; Budagov, J.; Buono, S.; Calôba, L. P.; Camin, D. V.; Canton, B.; Casado, P.; Cavalli, D.; Cavalli‐Sforza, M.; Cavasinni, V.; Chadelas, R.; Chase, R. L.; Chekhtman, A.; Chevaleyre, J.C.; Chevalley, J.L.; Чириков-Зорин, И.; Chlachidze, G.; Chollet, J.C.; Cobal, M.; Cogswell, F.; Colás, J.; Collot, J.; Cologna, S.; Constantinescu, S.; Costa, G.; Costanzo, D.; Cozzi, Luca; Crouau, M.; d’Argent, P.; Daudon, F.; David, M.; Davídek, T.; Dawson, J. W.; De, K.; Taille, C. de la; Prete, T. Del; Depommier, P.; Saintignon, P. de; Santo, A. De; Dinkespiller, B.; Girolamo, B. Di; Diţǎ, S.; Dolejší, J.; Doležal, Z.; Downing, Robert W.; Dugne, J.J.; Duval, P.Y.; Dzahini, D.; Efthymiopoulos, I.; Errede, D.; Errede, S.; Etienne, F.; Evans, H.; Fassnacht, P.; Fedyakin, N.N.; Ferrari, A.; Ferreira, P. M.; Ferrer, A.; Flaminio, V.; Fouchez, D.; Fournier, D.; Fumagalli, G.; Gallas, E. J.; Gaspar, M.; Gianotti, F.; Gildemeister, O.; Gingrich, D. M.; Glagolev, V.; Голубев, В. Б.; Gomes, A.; González, J. G.; Gordon, H. A.; Grabsky, V.; Hakopian, H.; Haney, M.; Hellman, S.; Henriques, A.; Holmgren, S. O.; Honoré, P. F.; Hostachy, Jean-Yves; Huston, J.; Ivanyushenkov, Y.; Jézéquel, S.; Johansson, Erik; Jon‐And, K.; Jones, Roger; Rozas, A. Juste; Kakurin, S.; Karapetian, G.; Karyukhin, A. N.; Khokhlov, Yu.A.; Klyukhin, V.; Kolomoets, V.; Kopikov, S. V.; Kostrikov, M.E.; Kovtun, V.; Kukhtin, V.; Kulagin, M.; Kulchitsky, Y.; Laborie, G.; Lami, S.; Lapin, V.; Lebedev, A. N.; Lefebvre, M.; Leflour, T.; Leitner, R.; León-Florián, E.; Leroy, C.; Suu, A. Le van; Li, J.; Liba, I.P.; Linossier, O.; Lokajı́ček, M.; Lomakin, Yu.F.; Lomakina, O.V.; Lund‐Jensen, B.; Mahout, G.; Maio, A.; Malyukov, S.; Mandelli, L.; Mansoulié, B.; Mapelli, L.; Marin, C.P.; Marroquin, F.; Martin, L.; Mazzanti, M.; Mazzoni, E.; Merritt, F. S.; Michel, B.; Miller, Richard H.; Minashvili, I. A.; Miotto, A.; Miralles, L.; Mnatsakanian, E.; Monnier, E.; Montarou, G.; Mornacchi, G.; Muanza, G. S.; Nagy, E.; Němeček, S.; Nessi, M.; Nicoleau, S.; Noppe, J.M.; Olivetto, C.; Orteu, S.; Aranda, C. Padilla; Pallin, D.; Pantea, D.; Parrour, G.; Pereira, A.; Perini, L.; Perlas, J. A.; Pétroff, P.; Pilcher, J. E.; Pinfold, J. L.; Plothow‐Besch, H.; Poggioli, L.; Poirot, S.; Polesello, G.; Price, L.E.; Protopopov, Yu.; Proudfoot, J.; Pukhov, O.; Radeka, V.; Rahm, D.; Reinmuth, G.; Renardy, J. F.; Renzoni, G.; Resconi, S.; Richards, R.; Riu, I.; Romanov, V. M.; Ronceux, B.; Rumyantsev, V.; Russakovich, N.; Sala, P.; Sanders, H.; Sauvage, G.; Savard, P.; Savoy-Navarro, A.; Sawyer, L.; Says, L. P.; Schaffer, A.C.; Scheel, C.; Schwemling, Ph.; Schwindling, J.; Seguin-Moreau, N.; Seixas, J. M.; Selldén, B.; Seman, M.; Semenov, A.; Senchishin, V.; Serin, L.; Shchelchkov, A.; Shevtsov, V.V.; Shochet, M. J.; Sidorov, V.; Simaitis, V.; Simion, S.; Sissakian, A. N.; Solodkov, A. A.; Sonderegger, P.; Soustružnı́k, K.; Stanek, R.; Starchenko, E. A.; Stephani, D.; Stephens, R. W.; Studenov, S.; Suk, M.; Surkov, A.; Tang, F.; Tardell, S.; Tas, P.; Teiger, J.; Teubert, F.; Thaler, J. J.; Tisserand, V.; Tisserant, S.; Tokár, S.; Topilin, N. D.; Trka, Z.; Turcot, A. S.; Turcotte, M.; Valkár, Š.; Vartapetian, A.; Vazeille, F.; Vichou, I.; Vinogradov, V. B.; Vorozhtsov, S.B.; Vuillemin, V.; Wagner, D. L.; White, A.; Wingerter-Seez, I.; Yamdagni, N.; Yarygin, G.; Yosef, C.; Zaitsev, A.; Zdrazil, M.; Zitoun, R.; Zolnierowski, Y.

doi:10.1016/s0168-9002(97)00075-2

Cited by 14 publications

(6 citation statements)

References 10 publications

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“…The benchmark reconstruction leads to the energy resolution of σ E /E = 55.4%/ √ E ⊕ 2.1%, with a constant term that satisfies the requirements. is compared with a simple sum of energy deposits in the ECAL and HCAL calibrated to the electromagnetic scale (pink circles) and results of the ATLAS test beam [13] (red line).…”

Section: Combined Performancementioning

confidence: 99%

Design and performance studies of a hadronic calorimeter for a FCC-hh experiment

Faltova

2018

J. Inst.

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Section: Combined Performancementioning

confidence: 99%

Design and performance studies of a hadronic calorimeter for a FCC-hh experiment

Faltova

2018

J. Inst.

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“…Similarly to the procedure in Refs. [11,21], the E dm term, which accounts for the energy loss in the dead material between the LAr and Tile calorimeters, is taken to be proportional to the geometrical mean of the energy released in the third depth of the electromagnetic compartment and the first depth of the hadronic compartment…”

Section: The E=h Methods Of Energy Reconstructionmentioning

confidence: 99%

Hadron energy reconstruction for the ATLAS calorimetry in the framework of the non-parametrical method ATLAS

Akhmadaliev¹,

Amaral²,

Ambrosini³

et al. 2002

Nuclear Instruments and Methods in Physics Research Section A:

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This paper discusses hadron energy reconstruction for the ATLAS barrel prototype combined calorimeter (consisting of a lead-liquid argon electromagnetic part and an iron-scintillator hadronic part) in the framework of the nonparametrical method. The non-parametrical method utilizes only the known e=h ratios and the electron calibration constants and does not require the determination of any parameters by a minimization technique. Thus, this technique lends itself to an easy use in a first level trigger. The reconstructed mean values of the hadron energies are within 71% of the true values and the fractional energy resolution is ½ð5873Þ%= ffiffiffi ffi E p þ ð2:570:3Þ%"ð1:770:2Þ=E: The value of the e=h ratio obtained for the electromagnetic compartment of the combined calorimeter is 1:7470:04 and agrees with the prediction that e=h > 1:66 for this electromagnetic calorimeter. Results of a study of the longitudinal hadronic shower development are also presented. The data have been taken in the H8 beam line of the CERN SPS using pions of energies from 10 to

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“…56. The obtained FCC-hh resolutions are given for B=0 T and compared to ATLAS testbeam results [48]. The benchmark method was also used by ATLAS in the combined testbeam for the energy combination of an electromagnetic liquid argon accordion calorimeter and an hadronic scintillating-tile calorimeter, however featuring a different ratio of active to passive absorber material with a Sci:Fe ratio of 1:4.7.…”

Section: Including Electronic Noise At the Cell Level Reconstructionmentioning

confidence: 99%

“…Right plot (b):The energy resolution of pions at η = 0.36, with B = 0 T is shown for 98 %, and 95 % lateral shower containment, corresponding to R < 0.3 and 0.17 respectively. The combined performance of EMB+HB is compared to ATLAS testbeam results[48].…”

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confidence: 99%

Calorimeters for the FCC-hh

Aleksa,

Allport,

Bosley

et al. 2019

Preprint

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The future proton-proton collider (FCC-hh) will deliver collisions at a center of mass energy up to √ s = 100 TeV at an unprecedented instantaneous luminosity of L = 3 10 35 cm −2 s −1 , resulting in extremely challenging radiation and luminosity conditions. By delivering an integrated luminosity of few tens of ab −1 , the FCC-hh will provide an unrivalled discovery potential for new physics. Requiring high sensitivity for resonant searches at masses up to tens of TeV imposes strong constraints on the design of the calorimeters. Resonant searches in final states containing jets, taus and electrons require both excellent energy resolution at multi-TeV energies as well as outstanding ability to resolve highly collimated decay products resulting from extreme boosts. In addition, the FCC-hh provides the unique opportunity to precisely measure the Higgs self-coupling in the di-photon and b-jets channel. Excellent photon and jet energy resolution at low energies as well as excellent angular resolution for pion background rejection are required in this challenging environment. This report describes the calorimeter studies for a multi-purpose detector at the FCChh. The calorimeter active components consist of Liquid Argon (LAr), scintillating plastic tiles (Tile) and Monolithic Active Pixel Sensors (MAPS) technologies. The technological choices, design considerations and achieved performances in full Geant4 simulations are discussed and presented.

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Results from a combined test of an electromagnetic liquid argon calorimeter with a hadronic scintillating-tile calorimeter

Cited by 14 publications

References 10 publications

Design and performance studies of a hadronic calorimeter for a FCC-hh experiment

Design and performance studies of a hadronic calorimeter for a FCC-hh experiment

Hadron energy reconstruction for the ATLAS calorimetry in the framework of the non-parametrical method ATLAS

Calorimeters for the FCC-hh

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