Hadron energy reconstruction for the ATLAS calorimetry in the framework of the nonparametrical method

Akhmadalev, S.; De Saintignon, P.; Jon-And, Kerstin B.; Moynot, M.; Mnatsakanian, E.; Tang, F.; Nicoleau, S.; Lomakin, Yu.; Maslennikov, A.; Thion, J.; Karyukhin, A.; Parrour, G.; Teiger, J.; Colas, J.; Spiwoks, R.; White, A.; Mornacchi, G.; Romance, J.B.; Sauvage, G.; Tikhonov, Y.; Sauvage, D.; Laborie, G.; Burdin, S.; Roldan, J.; Johansson, Erik Karl; Ivanyushenkov, Yu.; Proudfoot, J.; Valkar, S.; Efthymiopoulos, I.; Sellden, B.; Jenny, P.; Caloba, L.; Seman, M.; Sissakian, A.; Richer, J.P.; Jezequel, S.; Dolejsi, J.; Santos, J.; Linossier, O.; Canton, B.; Roda, C.; Krivkova, P.; Surkov, A.; Soustruznik, K.; Belymam, A.; Marin, C.P.; Santoni, C.; Li, J.; Fassi, F.; Gonzalez De La Hoz, S.; Monnier, E.; Le Flour, T.; Sanchis, E.; Soloviev, I.; Trka, Z.; Yosef, C.; Boldea, V.; Poirot, S.; Chalifour, M.; Evans, H.; Mazzanti, M.; Laforge, B.; Thaler, J.; Fumagalli, G.; Andrieux, M.L.; Mandelli, L.; Collot, Johann; Davidek, T.; Serin, L.; Wingerter-Seez, I.; Malyukov, S.; Says, L.P.; Tartarelli, F.; Lacour, D.; Kozlov, V.; Renzoni, G.; Schwindling, J.; Carvalho, J.; Lund-Jensen, B.; Bogush, A.; Vartapetian, A.; Le Dortz, O.; Rodier, S.; Liablin, M.; Makowiecki, D.; Kulagin, M.; Reinmuth, G.; Citterio, M.; Huston, J.; Chirikov-Zorin, I.; Baisin, L.; Marrocchesi, P.; Simaitis, V.; Berglund, S.; Gallas, E.; Aubert, Bernard; Pallin, D.; Dita, S.; Sawyer, L.; Fassnacht, P.; Dawson, J.; Auge, E.; Wolters, H.; Leitner, R.; Radeka, V.; Pantea, D.; Sonderegger, P.; Sala, P.; Niculescu, M.; Bazizi, K.; Kukhtin, V.; Fournier, D.; Perini, L.; Tokar, S.; Imbault, D.; Vazeille, F.; Lokajicek, M.; Tas, P.; Badaud, F.; Dugne, J.J.; Vuillemin, V.; Teubert, F.; Costa, G.; Bosman, M.; Lefebvre, M.; Errede, S.; Cavasinni, V.; Chevalley, J.L.; Klyukhin, V.; Soderqvist, J.; Parsons, J.; David, J.; Solodkov, Alexander A.; Varanda, M.J.; Muanza, G.S.; De la Taille, C.; Shaldaev, E.; Spano, F.; Kulchitsky, Y.; Cobal-Grassmann, Marina; Cogswell, F.; Ferrari, A.; Kakurin, S.; Gomes, A.; Di Girolamo, B.; Amaral, P.; Benchekroun, D.; Jones, R.; Camin, D.V.; Bohm, C.; Lopez Amengual, J.M.; Romanov, V.; Merritt, F.; Suk, M.; Stanek, R.; Holmgren, S.; Sykora, I.; Miralles, L.; Khokhlov, Yu.A.; Schwemling, P.; Martin, P.; Dodd, J.; Tisserant, S.; Plothow-Besch, H.; Budagov, J.; Gonzalez, V.; Poggioli, L.; Bromberg, C.; Vorozhtsov, S.; Breton, D.; Ferrer, A.; Schaffer, A.C.; Price, L.; Minashvili, I.; Crouau, M.; Onofre, A.; Yamdagni, N.; Paoletti, R.; Topilin, N.; Hostachy, J.Y.; Simion, S.; Tardell, S.; Lapin, V.; Nayman, P.; Giokaris, N.; Dinkespiller, B.; Dzahini, D.; Del Prete, T.; Hoummada, A.; Chadelas, R.; Higon, E.; Semenov, A.; Perlas, J.A.; Lobkowicz, F.; Glebov, V.; Lami, S.; Flaminio, V.; Lissauer, D.; Starchenko, E.; Zaitsev, A.; Snopkov, R.; Bazan, A.; Riu, I.; Shochet, M.; Hakopian, H.; Stephens, R.; Michel, B.; Zitoun, R.; Blanchot, G.; Marroquin, F.; Castillo, M.V.; Noppe, J.M.; Puzo, P.; Stavina, P.; Mapelli, L.; Protopopov, Y.; Richards, R.; Anderson, K.; Eynard, G.; Kolachev, G.; Grabsky, V.; Cologna, S.; Nemecek, S.; Maio, A.; Cavalli, D.; Seidl, W.; Cavalli-Sforza, M.; Constantinescu, S.; David, M.; Pinhao, J.; Perrodo, P.; De, K.; Del Peso, J.; Shekhtman, Lev I.; Soloviev, A.; Bouhemaid, N.; Mataix, L.; Camarena, F.; Sidorov, V.; Kopikov, S.; Mansoulie, B.; Casado, P.; Amorim, A.; Sanders, H.; Henriques, A.; Giakoumopoulou, V.; Park, I.C.; Mazzoni, E.; Grauges, E.; Takai, H.; Juste, A.; Brette, P.; Kuzmin, M.; Ambrosini, G.; Hebrard, C.; Seixas, J.M.; Caprini, M.; Massol, N.; Barreiro, F.; Cleland, W.E.; Leltchouk, M.; Rahm, D.; Miller, R.; Gaspar, M.; Glagolev, V.; Khubua, J.; Turcotte, M.; Rossel, F.; Costanzo, D.; Gianotti, F.; Rescia, S.; Zolnierowski, Y.P.; Vinogradov, V.; Errede, D.; Seguin-Moreau, N.; Gildemeister, O.; Bonivento, W.; Kostrikov, M.; Haney, M.; Chlachidze, G.; Nessi, M.; Wielers, M.; Downing, R.; Berset, J.C.; Silva, J.; Labarga, L.; Montarou, G.; Hervas, L.; Resconi, S.; Pereira, A.; Pilcher, J.; Dolezal, Z.; Romero, P.; Daudon, F.; Russakovich, N.; Clement, C.; Battistoni, G.; Grenier, P.; Vichou, I.

doi:10.1016/S0168-9002(01)01229-3

000567322 001__ 567322
000567322 003__ SzGeCERN
000567322 005__ 20210715034623.0
000567322 0247_ $$2DOI$$a10.1016/S0168-9002(01)01229-3
000567322 0248_ $$aoai:cds.cern.ch:567322$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
000567322 035__ $$9CERCER$$a2325198
000567322 035__ $$9INSPEC$$a7278073
000567322 035__ $$9CERN annual report$$a2002-3.0801
000567322 035__ $$9Inspire$$a554879
000567322 037__ $$9arXiv$$ahep-ex/0104002$$chep-ex
000567322 041__ $$aeng
000567322 100__ $$aAkhmadalev, S.
000567322 245__ $$aHadron energy reconstruction for the ATLAS calorimetry in the framework of the nonparametrical method
000567322 246__ $$aA TOROIDAL LHC APPARATUS
000567322 246__ $$aLARGE HADRON COLLIDER
000567322 260__ $$c2002
000567322 269__ $$c2001-04
000567322 300__ $$a33 p
000567322 500__ $$9arXiv$$a33 pages, 13 figures, Will be published in NIMA
000567322 520__ $$aThis 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 nonparametrical 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 +or-1% of the true values and the fractional energy resolution is [(58+or-3)%/ square root E+(2.5+or-0.3)%](+)(1.7+or-0.2)/E. The value of the e/h ratio obtained for the electromagnetic compartment of the combined calorimeter is 1.74+or-0.04 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 300 GeV. (32 refs).
000567322 520__ $$9arXiv$$aThis 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 non-parametrical 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 $\pm 1%$ of the true values and the fractional energy resolution is $[(58\pm3)% /\sqrt{E}+(2.5\pm0.3)%]\oplus (1.7\pm0.2)/E$. The value of the $e/h$ ratio obtained for the electromagnetic compartment of the combined calorimeter is $1.74\pm0.04$ and agrees with the prediction that $e/h > 1.7$ 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 300 GeV.
000567322 595__ $$aSIS INSP2002
000567322 595__ $$i7278073
000567322 65017 $$2SzGeCERN$$aDetectors and Experimental Techniques
000567322 690C_ $$aARTICLE
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000567322 694__ $$9INSPEC$$aA2940M (Scintillation detectors; scintillators and photomultipliers)
000567322 694__ $$9INSPEC$$aA2970G (Energy loss and energy range relations in radiation measurement)
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000567322 694__ $$9INSPEC$$aCI Ar el; Pb el; Fe el
000567322 694__ $$9INSPEC$$aNI electron volt energy: 1
000567322 695__ $$9INSPEC$$acalibration
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000567322 695__ $$9INSPEC$$aliquid-ionisation-chambers
000567322 695__ $$9INSPEC$$aparticle-calorimetry
000567322 695__ $$9INSPEC$$asolid-scintillation-detectors
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000567322 700__ $$aSolodkov, Alexander A.$$iINSPIRE-00127668
000567322 700__ $$aSoloviev, A.
000567322 700__ $$aSoloviev, I.$$iINSPIRE-00390496
000567322 700__ $$aSonderegger, P.
000567322 700__ $$aSoustruznik, K.
000567322 700__ $$aSpano, F.$$iINSPIRE-00051714
000567322 700__ $$aSpiwoks, R.$$iINSPIRE-00223859
000567322 700__ $$aStanek, R.$$iINSPIRE-00128391
000567322 700__ $$aStarchenko, E.$$iINSPIRE-00223911
000567322 700__ $$aStavina, P.$$iINSPIRE-00223944
000567322 700__ $$aStephens, R.
000567322 700__ $$aSuk, M.$$iINSPIRE-00224089
000567322 700__ $$aSurkov, A.
000567322 700__ $$aSykora, I.$$iINSPIRE-00224134
000567322 700__ $$aTakai, H.$$iINSPIRE-99155656
000567322 700__ $$aTang, F.$$iINSPIRE-00380536
000567322 700__ $$aTardell, S.
000567322 700__ $$aTartarelli, F.$$iINSPIRE-00130743
000567322 700__ $$aTas, P.$$iINSPIRE-00306326
000567322 700__ $$aTeiger, J.
000567322 700__ $$aTeubert, F.
000567322 700__ $$aThaler, J.
000567322 700__ $$aThion, J.
000567322 700__ $$aTikhonov, Y.$$iINSPIRE-00198040
000567322 700__ $$aTisserant, S.$$iINSPIRE-00131587
000567322 700__ $$aTokar, S.$$iINSPIRE-00131686
000567322 700__ $$aTopilin, N.$$iINSPIRE-00224555
000567322 700__ $$aTrka, Z.
000567322 700__ $$aTurcotte, M.
000567322 700__ $$aValkar, S.$$iINSPIRE-00224924
000567322 700__ $$aVaranda, M.J.
000567322 700__ $$aVartapetian, A.$$iINSPIRE-00225055
000567322 700__ $$aVazeille, F.$$iINSPIRE-00225072
000567322 700__ $$aVichou, I.$$iINSPIRE-00161358
000567322 700__ $$aVinogradov, V.$$iINSPIRE-00227012
000567322 700__ $$aVorozhtsov, S.
000567322 700__ $$aVuillemin, V.
000567322 700__ $$aWhite, A.$$iINSPIRE-00013505
000567322 700__ $$aWielers, M.$$iINSPIRE-00225743
000567322 700__ $$aWingerter-Seez, I.$$iINSPIRE-00136245
000567322 700__ $$aWolters, H.$$iINSPIRE-00225832
000567322 700__ $$aYamdagni, N.
000567322 700__ $$aYosef, C.
000567322 700__ $$aZaitsev, A.$$iINSPIRE-00170475
000567322 700__ $$aZitoun, R.$$iINSPIRE-00233264
000567322 700__ $$aZolnierowski, Y.P.$$iINSPIRE-00233288
000567322 710__ $$gATLAS Collaboration
000567322 710__ $$5EP
000567322 773__ $$c508-23$$n2-3$$pNucl. Instrum. Methods Phys. Res., A$$v480$$y2002
000567322 8564_ $$81444890$$s28577$$uhttps://cds.cern.ch/record/567322/files/comb96_1.png$$y00002 Schematic layout of the experimental setup for the combined LAr and Tile calorimeters run (side view). The S3 and S4 are scintillation counters, the BC3 is a beam proportional chamber, and the midsampler and the ``muon wall'' are scintillation hodoscopes.
000567322 8564_ $$81444891$$s11655$$uhttps://cds.cern.ch/record/567322/files/epi_50.png$$y00005 The distributions of the $(e/\pi)_{LAr}$ ratio for beam energies of 20 and 50 GeV (top row, left to right), and beam energies of 100 and 300 GeV (bottom row, left to right).
000567322 8564_ $$81444892$$s511517$$uhttps://cds.cern.ch/record/567322/files/arXiv:hep-ex_0104002.pdf
000567322 8564_ $$81444893$$s16433$$uhttps://cds.cern.ch/record/567322/files/vpro-fig-our-long-conb-bock-26.png$$y00018 The experimental differential mean longitudinal energy depositions at 10 GeV (crosses), 20 GeV (black top triangles), 40 GeV (open squares), 50 GeV (black squares), 80 GeV (open circles), 100 GeV (black circles), 150 GeV (stars), 300 GeV (black bottom triangles) energies as a function of the longitudinal coordinate $z$ in units $\lambda_{\pi}$ for the combined calorimeter and the results of the description by the modified parameterization for the equation (\ref{elong03}).
000567322 8564_ $$81444894$$s18477$$uhttps://cds.cern.ch/record/567322/files/vpro-fig-our-long-conb-bock-27.png$$y00017 The comparison between the experimental differential mean energy depositions at 10 GeV (crosses), 20 GeV (black top triangles), 40 GeV (open squares), 50 GeV (black squares), 80 GeV (open circles), 100 GeV (black circles), 150 GeV (stars), 300 GeV (black bottom triangles) and the calculated curves (\ref{elong03}) as a function of the longitudinal coordinate $z$ in units $\lambda_{\pi}$. The errors on the data points are the errors of the mean values and there are within symbols size.
000567322 8564_ $$81444895$$s12551$$uhttps://cds.cern.ch/record/567322/files/epi_20.png$$y00004 The distributions of the $(e/\pi)_{LAr}$ ratio for beam energies of 20 and 50 GeV (top row, left to right), and beam energies of 100 and 300 GeV (bottom row, left to right).
000567322 8564_ $$81444896$$s12729$$uhttps://cds.cern.ch/record/567322/files/energy_50.png$$y00012 The energy distributions for beam energies of 20 and 50 GeV (top row, left to right), and beam energies of 100 and 300 GeV (bottom row, left to right).
000567322 8564_ $$81444897$$s12411$$uhttps://cds.cern.ch/record/567322/files/energy_100.png$$y00013 The energy distributions for beam energies of 20 and 50 GeV (top row, left to right), and beam energies of 100 and 300 GeV (bottom row, left to right).
000567322 8564_ $$81444898$$s9707$$uhttps://cds.cern.ch/record/567322/files/epi_300.png$$y00007 The distributions of the $(e/\pi)_{LAr}$ ratio for beam energies of 20 and 50 GeV (top row, left to right), and beam energies of 100 and 300 GeV (bottom row, left to right).
000567322 8564_ $$81444899$$s105359$$uhttps://cds.cern.ch/record/567322/files/chapter1_fig3.png$$y00001 Three-dimensional cutaway view of the ATLAS calorimeters.
000567322 8564_ $$81444900$$s11676$$uhttps://cds.cern.ch/record/567322/files/energy_20.png$$y00011 The energy distributions for beam energies of 20 and 50 GeV (top row, left to right), and beam energies of 100 and 300 GeV (bottom row, left to right).
000567322 8564_ $$81444901$$s11588$$uhttps://cds.cern.ch/record/567322/files/ehl_rd3_0.png$$y00009 The $(e/\pi)_{LAr}$ ratios as a function of the beam energy. for $e/h$ method (black circles) and for weighting method (open circles for \cite{stipcevic93} and open squares for \cite{Gingrich95}). The lines are the result of a fit of equations (\ref{ev10}) and (\ref{ev10-0}) with free $e/h$ parameter and $k=0.11$: solid line is for our data, dashed line is for the \cite{stipcevic93} data and dash-doted line is for the \cite{Gingrich95} data.
000567322 8564_ $$81444902$$s19155$$uhttps://cds.cern.ch/record/567322/files/lin-comb-s-01.png$$y00016 The energy resolutions obtained with the $e/h$ method (black circles), the benchmark method (crosses) and the cells weighting method (circles).
000567322 8564_ $$81444903$$s11680$$uhttps://cds.cern.ch/record/567322/files/lar-tile-en.png$$y00019 Energy deposition (percentage) in the LAr and Tile calorimeters at different beam energies. The circles (squares) are the measured energy depositions in the LAr (Tile) calorimeter, the diamonds (crosses) are the calculated energy depositions.
000567322 8564_ $$81444904$$s12250$$uhttps://cds.cern.ch/record/567322/files/energy_300.png$$y00014 The energy distributions for beam energies of 20 and 50 GeV (top row, left to right), and beam energies of 100 and 300 GeV (bottom row, left to right).
000567322 8564_ $$81444905$$s8505$$uhttps://cds.cern.ch/record/567322/files/lin-comb-010.png$$y00010 Energy linearity as a function of the beam energy for the $e/h$ method obtained using the iteration procedure with $\epsilon = 0.1\%$ (black circles) and with the first approximation (open circles).
000567322 8564_ $$81444906$$s33182$$uhttps://cds.cern.ch/record/567322/files/pro-fig28tp0.png$$y00003 Conceptual design of a Tile calorimeter module.
000567322 8564_ $$81444907$$s10806$$uhttps://cds.cern.ch/record/567322/files/epi_100.png$$y00006 The distributions of the $(e/\pi)_{LAr}$ ratio for beam energies of 20 and 50 GeV (top row, left to right), and beam energies of 100 and 300 GeV (bottom row, left to right).
000567322 8564_ $$81444908$$s9094$$uhttps://cds.cern.ch/record/567322/files/ehl.png$$y00008 The mean value of the $(e/\pi)_{LAr}$ ratio as a function of the beam energy. The curve is the result of a fit of equations (\ref{ev10}) and (\ref{ev10-0}).
000567322 8564_ $$81444909$$s10544$$uhttps://cds.cern.ch/record/567322/files/lin-comb-001.png$$y00015 Energy linearity as a function of the beam energy for the $e/h$ method (black circles) and the cells weighting method (open circles).
000567322 8564_ $$82306891$$s9563$$uhttps://cds.cern.ch/record/567322/files/fig00000.png$$y00000 noimg: Mean reconstructed energy, energy resolution and fractional energy resolution for the various beam energies.: The differential mean energy depositions $\Delta E/ \Delta z$ ($GeV/\lambda_\pi$) as a function of the longitudinal coordinate $z$ for the various beam energies.
000567322 901__ $$uCERN
000567322 916__ $$sh$$w200252$$ya2002
000567322 960__ $$a13
000567322 961__ $$c20100928$$h1517$$lCER01$$x20020706
000567322 963__ $$aPUBLIC
000567322 970__ $$a002325198CER
000567322 980__ $$aARTICLE

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