Dr Elizabeth Gallas: Publications

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

Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 387:3 (1997) 333-351

Authors:

Z Ajaltouni, F Albiol, A Alifanov, P Amaral, G Ambrosini, A Amorim, K Anderson, A Astvatsaturov, B Aubert, E Augé, D Autiero, G Azuelos, F Badaud, L Baisin, G Battistoni, A Bazan, C Bee, G Bellettini, S Berglund, JC Berset, C Blaj, G Blanchot, E Blucher, A Bogush, C Bohm, V Boldea, O Borisov, M Bosnian, N Bouhemaid, P Brette, C Bromberg, M Brossard, J Budagov, S Buono, L Caloba, DV Camin, B Canton, P Casado, D Cavalli, M Cavalli-Sforza, V Cavasinni, R Chadelas, R Chase, A Chekhtman, JC Chevaleyre, JL Chevalley, I Chirikov-Zorin, G Chlachidze, JC Chollet, M Cobal, F Cogswell, J Colas, J Collot, S Cologna, S Constantinescu, G Costa, D Costanzo, L Cozzi, M Crouau, P Dargent, F Daudon, M David, T Davidek, J Dawson, K De, C de la Taille, T Del Prete, P Depommier, P de Saintignon, A de Santo, B Dinkespiller, B di Girolamo, S Dita, J Dolejsi, Z Dolezal, R Downing, JJ Dugne, PY Duval, D Dzahini, I Efthymiopoulos, D Errede, S Errede, F Etienne, H Evans, P Fassnacht, N Fedyakin, A Ferrari, P Fcrreira, A Ferrer, V Flaminio, D Fouchez, D Fournier, G Fumagalli, E Gallas, M Gaspar, F Gianotti, O Gildemeister, DM Gingrich, V Glagolev, V Golubev

Abstract:

The first combined test of an electromagnetic liquid argon accordion calorimeter and a hadronic scintillating-tile calorimeter was carried out at the CERN SPS. These devices are prototypes of the barrel calorimeter of the future ATLAS experiment at the LHC. The energy resolution of pions in the energy range from 20 to 300 GeV at an incident angle θ of about 11c is well-described by the expression σ/E = ((46.5 ± 6.0)%/√E + (1.2 ± 0.3)%) ⊗ (3.2 ± 0.4)GeV/E. Shower profiles, shower leakage, and the angular resolution of hadronic showers were also studied.

A measurement of the energy loss spectrum of 150 GeV muons in iron

Zeitschrift Fur Physik C Particles and Fields 73:3 (1997) 455-463

Authors:

E Berger, R Blair, J Dawson, T Fuess, V Guarino, N Hill, S Magill, E May, L Nodulman, L Price, J Proudfoot, R Stanek, D Underwood, R Wagner, B Wicklund, G Blanchot, M Bosman, P Casado, M Cavalli-Sforza, I Efthymiopoulos, Y Ivanyushenkov, A Juste, L Miralles, S Orteu, C Padilla, JA Perlas, I Riu, B Ronceux, F Teubert, R Arsenescu, S Constantinescu, C Blaj, V Boldea, S Dita, M Cobal, O Gildemeister, M Nessi, A Henriques, L Poggioli, P Sonderegger, G Karapetian, K Anderson, E Blucher, H Evans, F Merritt, J Pilcher, H Sanders, M Shochet, F Tang, A Turcot, D Wagner, Z Ajaltouni, F Badaud, N Bouhemaid, P Brette, M Brassard, R Chadelas, JC Chevaleyre, M Crouau, F Daudon, JJ Dugne, B Michel, G Montarou, GS Muanza, D Pallin, H Plothow-Besch, S Poirot, G Reinmuth, LP Says, F Vazeille, A Astvatsaturov, O Borisov, J Budagov, I Chirikov-Zorin, G Chlachidze, V Glagolev, S Kakurin, V Kolomoets, V Kovtun, V Kukhtin, A Lebedev, I Liba, O Lomakina, Y Lomakin, S Malyukov, I Minashvili, D Pantea, O Pukhov, V Romanov, N Russakovich, V Senchishin, A Semenov, A Sissakian, A Shchelchkov, V Shevtsov, S Studenov, S Tokar, N Topilin, V Vinogradov, S Vorozhtsov

Abstract:

The energy loss spectrum of 150 GeV muons has been measured with a prototype of the ATLAS hadron calorimeter in the H8 beam of the CERN SPS. The differential probability dP/dυ per radiation length of a fractional energy loss υ = ΔEμ/Eμ has been measured in the range υ = 0.01 ÷ 0.95; it is compared with the theoretical predictions for energy losses due to bremsstrahlung and production of electron-positron pairs or of energetic knock-on electrons. The integrated probability ∫0.01^0.95(dP/dυ)dυ is (1.610 ± 0.015stat ±0 .105syst)·10^-3 in agreement with the theoretical predictions 1.556·10^-3 and 1.619·10^-3. Agreement with theory is also found in two intervals of υ where production of electron-positron pairs and knock-on electrons dominates. In the region of bremsstrahlung dominance (υ = 0.12 ÷ 0.95) the measured integrated probability (1.160 ± 0.040stat ± 0.075syst)·10^-4 is in agreement with the theoretical value of 1.185·10^-4, obtained using the Petrukhin and Shestakov description of the bremsstrahlung process. The same result is about 3.6 standard deviations (defined as the quadratic sum of statistical and systematic errors) lower than the theoretical prediction of 1.472·10^-4, obtained using Tsai's description of bremsstrahlung. © Springer-Verlag 1997.

Direct measurement of the top quark mass

Physical Review Letters 79:7 (1997) 1197-1202

Authors:

S Abachi, B Abbott, M Abolins, BS Acharya, I Adam, DL Adams, M Adams, S Ahn, H Aihara, GA Alves, E Amidi, N Amos, EW Anderson, R Astur, MM Baarmand, A Baden, V Balamurali, J Balderston, B Baldin, S Banerjee, J Bantly, E Barberis, JF Bartlett, K Bazizi, A Belyaev, SB Beri, I Bertram, VA Bezzubov, PC Bhat, V Bhatnagar, M Bhattacharjee, N Biswas, G Blazey, S Blessing, P Bloom, A Boehnlein, NI Bojko, F Borcherding, J Borders, C Boswell, A Brandt, R Brock, A Bross, D Buchholz, VS Burtovoi, JM Butler, W Carvalho, D Casey, H Castilla-Valdez, D Chakraborty, SM Chang, SV Chekulaev, LP Chen, W Chen, S Choi, S Chopra, BC Choudhary, JH Christenson, M Chung, D Claes, AR Clark, WG Cobau, J Cochran, WE Cooper, C Cretsinger, D Cullen-Vidal, MAC Cummings, D Cutts, OI Dahl, K Davis, K De, K Del Signore, M Demarteau, D Denisov, SP Denisov, HT Diehl, M Diesburg, G Di Loreto, P Draper, J Drinkard, Y Ducros, LV Dudko, SR Dugad, D Edmunds, J Ellison, VD Elvira, R Engelmann, S Eno, G Eppley, P Ermolov, OV Eroshin, VN Evdokimov, T Fahland, M Fatyga, MK Fatyga, J Featherly, S Feher, D Fein, T Ferbel, G Finocchiaro

Abstract:

We measure the top quark mass mt t¯t using pairs produced in the D0 detector by √s = 1.8 TeV p ¯p collisions in a 125pb^-1 exposure at the Fermilab Tevatron. We make a two constraint fit to mt in t¯t → b W⁺ ¯��^- final states with one W decaying to q¯q and the other to ev or μ v. Events are binned in fit mass versus a measure of probability for events to be signal rather than background. Likelihood fits to the data yield mt = 17.3 ± 5.6 (stat) ± 6.2(syst) GeV/c². © 1998 The American Physical Society.

Measurement of the top quark pair production cross section in p¯p collisions

Physical Review Letters 79:7 (1997) 1203-1208

Authors:

S Abachi, B Abbott, M Abolins, BS Acharya, I Adam, DL Adams, M Adams, S Ahn, H Aihara, GA Alves, E Amidi, N Amos, EW Anderson, R Astur, MM Baarmand, A Baden, V Balamurali, J Balderston, B Baldin, S Banerjee, J Bantly, JF Bartlett, K Bazizi, A Belyaev, SB Beri, I Bertram, VA Bezzubov, PC Bhat, V Bhatnagar, M Bhattacharjee, N Biswas, G Blazey, S Blessing, P Bloom, A Boehnlein, NI Bojko, F Borcherding, J Borders, C Boswell, A Brandt, R Brock, A Bross, D Buchholz, VS Burtovoi, JM Butler, W Carvalho, D Casey, Z Casilum, H Castilla-Valdez, D Chakraborty, SM Chang, SV Chekulaev, LP Chen, W Chen, S Choi, S Chopra, BC Choudhary, JH Christenson, M Chung, D Claes, AR Clark, WG Cobau, J Cochran, WE Cooper, C Cretsinger, D Cullen-Vidal, MAC Cumings, D Cutts, OI Dahl, K Davis, K De, K Del Signore, M Demarteau, D Denisov, SP Denisov, HT Diehl, M Diesburg, G Di Loreto, P Draper, J Drinkard, Y Ducros, LV Dudko, SR Dugad, D Edmunds, J Ellison, VD Elvira, R Engelmann, S Eno, G Eppley, P Ermolov, OV Eroshin, VN Evdokimov, T Fahland, M Fatyga, MK Fatyga, J Featherly, S Feher, D Fein, T Ferbel, G Finocchiaro

Abstract:

We present a measurement of the t¯t production cross section in p¯p collisions at √s=1.8TeV by the D0 experiment at the Fermilab Tevatron. The measurement is based on data from an integrated luminosity of approximately 125pb−1 accumulated during the 1992–1996 collider run. We observe 39 t¯t candidate events in the dilepton and lepton+jets decay channels with an expected background of 13.7 ± 2.2 events. For a top quark mass of 173.3 GeV/c2, we measure the t¯t production cross section to be 5.5 ± 1.8 pb. © 1997 The American Physical Society.

Search for a Fourth Generation Charge -1/3 Quark via Flavor Changing Neutral Current Decay

Physical Review Letters 78:20 (1997) 3818-3823

Authors:

S Abachi, B Abbott, M Abolins, BS Acharya, I Adam, DL Adams, M Adams, S Ahn, H Aihara, GA Alves, E Amidi, N Amos, EW Anderson, R Astur, MM Baarmand, A Baden, V Balamurali, J Balderston, B Baldin, S Banerjee, J Bantly, JF Bartlett, K Bazizi, A Belyaev, SB Beri, I Bertram, VA Bezzubov, PC Bhat, V Bhatnagar, M Bhattacharjee, N Biswas, G Blazey, S Blessing, P Bloom, A Boehnlein, NI Bojko, F Borcherding, J Borders, C Boswell, R Brock, A Bross, D Buchholz, VS Burtovoi, JM Butler, W Carvalho, D Casey, H Castilla-Valdez, D Chakraborty, SM Chang, SV Chekulaev, LP Chen, W Chen, S Choi, S Chopra, BC Choudhary, JH Christenson, M Chung, D Claes, AR Clark, WG Cobau, J Cochran, WE Cooper, C Cretsinger, D Cullen-Vidal, MAC Cummings, D Cutts, OI Dahl, K De, K Del Signore, M Demarteau, D Denisov, SP Denisov, HT Diehl, M Diesburg, G Di Loreto, P Draper, J Drinkard, J Alitti, LV Dudko, SR Dugad, D Edmunds, J Ellison, VD Elvira, R Engelmann, S Eno, G Eppley, P Ermolov, OV Eroshin, VN Evdokimov, T Fahland, M Fatyga, MK Fatyga, J Featherly, S Feher, D Fein, T Ferbel, G Finocchiaro, HE Fisk, Y Fisyak

Abstract:

We report on a search for pair production of a fourth generation charge -1/3 quark (b’) in pp collisions at s = 1.8 TeV by the DØ experiment at the Fermilab Tevatron using an integrated luminosity of 93 pb-1. Both b’ quarks are assumed to decay via flavor changing neutral currents (FCNC). The search uses the signatures γ + 3 jets + μ-tag and 2γ + 2 jets. We see no significant excess of events over the expected background. We place an upper limit on the production cross section times branching fraction that is well below theoretical expectations for a b’ decaying exclusively via FCNC for b’ masses up to mz + mb. © 1996 American Physical Society.

51��