@article{3081621,
    title = "Hadron energy reconstruction for the ATLAS calorimetry in the framework
of the non-parametrical method",
    author = "Akhmadaliev, S and Amaral, P and Ambrosini, G and Amorim, A and and Anderson, K and Andrieux, ML and Aubert, B and Auge, E and Badaud, F and and Baisin, L and Barreiro, F and Battistoni, G and Bazan, A and Bazizi, K and and Belymam, A and Benchckroun, D and Berglund, S and Berset, JC and and Blanchot, G and Bogush, A and Bohm, C and Boldea, V and Bonivento, W and and Bosman, M and Bouhemaid, N and Breton, D and Brette, P and Bromberg, C and and Budagov, J and Burdin, S and Caloba, L and Camarena, F and Camin, DV and and Canton, B and Caprini, M and Carvalho, J and Casado, P and Castillo, and MV and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Chadelas, R and and Chalifour, M and Chekhtman, L and Chevalley, JL and Chirikov-Zorin, and I and Chlachidze, G and Citterio, M and Cleland, WE and Clement, C and and Cobal, M and Cogswell, F and Colas, J and Collot, J and Cologna, S and and Constantinescu, S and Costa, G and Costanzo, D and Crouau, M and Daudon, and F and David, J and David, M and Davidek, T and Dawson, J and De, K and and de la Taille, C and Del Peso, J and Del Prete, T and de Saintignon, P and and Di Girolamo, B and Dinkespiller, B and Dita, S and Dodd, J and and Dolejsi, J and Dolezal, Z and Downing, R and Dugne, JJ and Dzahini, D and and Efthymiopoulos, I and Errede, D and Errede, S and Evans, H and and Eynard, G and Fassi, F and Fassnacht, P and Ferrari, A and Ferrari, A and and Ferrer, A and Flaminio, V and Fournier, D and Fumagalli, G and and Gallas, E and Gaspar, MG and Giakoumopoulou, V and Gianotti, F and and Gildemeister, O and Giokaris, N and Glagolev, V and Glebov, V and Gomes, and A and Gonzalez, V and De la Hoz, SG and Grabsky, V and Grauges, E and and Grenier, P and Hakopian, H and Haney, M and Hebrard, C and Henriques, A and and Hervas, L and Higon, E and Holmgren, S and Hostachy, JY and and Hoummada, A and Huston, J and Imbault, D and Ivanyushenkov, Y and and Jezequel, S and Johansson, E and Jon-And, K and Jones, R and Juste, A and and Kakurin, S and Karyukhin, A and Khokhlov, Y and Khubua, J and and Klyukhin, V and Kolachev, G and Kopikov, S and Kostrikov, M and Kozlov, and V and Krivkova, P and Kukhtin, V and Kulagin, M and Kulchitsky, Y and and Kuzmin, M and Labarga, L and Laborie, G and Lacour, D and Laforge, B and and Lami, S and Lapin, V and Le Dortz, O and Lefebvre, M and Le Flour, T and and Leitner, R and Leltchouk, M and Li, J and Liablin, M and Linossier, O and and Lissauer, D and Lobkowicz, F and Lokajicek, M and Lomakin, Y and and Amengual, JML and Lund-Jensen, B and Maio, A and Makowiecki, D and and Malyukov, S and Mandelli, L and Mansoulie, B and Mapelli, L and Marin, and CP and Marrocchesi, P and Marroquim, F and Martin, P and Maslennikov, A and and Massol, N and Mataix, L and Mazzanti, M and Mazzoni, E and Merritt, and F and Michel, B and Miller, R and Minashvili, I and Miralles, L and and Mnatsakanian, E and Monnier, E and Montarou, G and Mornacchi, G and and Moynot, M and Muanza, GS and Nayman, P and Nemecek, S and Nessi, M and and Nicoleau, S and Niculescu, M and Noppe, JM and Onofre, A and Pallin, D and and Pantea, D and Paoletti, R and Park, IC and Parrour, G and Parsons, J and and Pereira, A and Perini, L and Perlas, JA and Perrodo, P and Pilcher, and J and Pinhao, J and Plothow-Besch, H and Poggioli, L and Poirot, S and and Price, L and Protopopov, Y and Proudfoot, J and Puzo, P and Radeka, V and and Rahm, D and Reinmuth, G and Renzoni, G and Resica, S and Resconi, S and and Richards, R and Richer, JP and Roda, C and Rodier, S and Roldan, J and and Romance, JB and Romance, V and Romero, P and Rossel, F and and Russakovich, N and Sala, P and Sanchis, E and Sanders, H and Santoni, C and and Santos, J and Sauvage, D and Sauvage, G and Sawyer, L and Says, LP and and Schaffer, AC and Schwemling, P and Schwindling, J and Seguin-Moreau, and N and Seidl, W and Seixas, JM and Sellden, B and Seman, M and Semenov, A and and Serin, L and Shaldaev, E and Shochet, M and Sidorov, V and Silva, J and and Simaitis, V and Simion, S and Sissakian, A and Snopkov, R and and Soderqvist, J and Solodkov, A and Soloviev, A and Soloviev, I and and Sonderegger, P and Soustruznik, K and Spano, F and Spiwoks, R and and Stanek, R and Starchenko, E and Stavina, P and Stephens, R and Suk, M and and Surkov, A and Sykora, I and Takai, H and Tang, F and Tardell, S and and Tartarelli, F and Tas, P and Teiger, J and Thaler, J and Thion, J and and Tikhonov, Y and Tisserant, S and Tokar, S and Topilin, N and Trka, Z and and Turcotte, M and Valkar, S and Varanda, MJ and Vartapetian, A and and Vazeille, F and Vichou, I and Vinogradov, V and Vorozhtsov, S and and Vuillemin, V and White, A and Wielers, M and Wingerter-Seez, I and and Wolters, H and Yamdagni, N and Yosef, C and Zaitsev, A and Zitoun, R and and Zolnierowski, YP",
    journal = "NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION
A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT",
    year = "2002",
    volume = "480",
    number = "2-3",
    pages = "508-523",
    publisher = "Elsevier",
    doi = "10.1016/S0168-9002(01)01229-3",
    keywords = "calorimetry; combined calorimeter; shower counter; compensation; energy
measurement; computer data analysis",
    abstract = "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 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 +/-1% of the true values and the fractional energy
resolution is [(58+/-3)%/rootE+(2.5+/-0.3)%]circle
plus(1.7+/-0.2)/E. The value of the e/h ratio obtained for the
electromagnetic compartment of the combined calorimeter is 1.74+/-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. (C)
2002 Elsevier Science B.V. All rights reserved."
}