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Table 67

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Phillips, H.T.;Pierre, F.;Pimenta, M.;Abreu, P.;Adam, W.;Adye, T.;Adzic, P.;Albrecht, Z.;Alderweireld, T.;Alekseev, G.D.;Alemany, R.;Allmendinger, T.;Allport, P.P.;Almehed, S.;Amaldi, U.;Amapane, N.;Amato, S.;Anassontzis, E.G.;Andersson, P.;Andreazza, A.;Andringa, S.;Antilogus, P.;Apel, W.D.;Arnoud, Y.;Asman, B.;Augustin, J.E.;Augustinus, A.;Baillon, P.;Bambade, P.;Barao, F.;Barbiellini, G.;Barbier, R.;Bardin, D.Yu.;Barker, G.J.;Baroncelli, A.;Battaglia, M.;Baubillier, M.;Becks, K.H.;Begalli, M.;Behrmann, A.;Beilliere, P.;Belokopytov, Yu.;Benekos, N.C.;Benvenuti, A.C.;Berat, C.;Berggren, M.;Bertini, D.;Bertrand, D.;Besancon, M.;Bigi, M.;Bilenky, Mikhail S.;Bizouard, M.A.;Bloch, D.;Blom, H.M.;Bonesini, M.;Bonivento, W.;Boonekamp, M.;Booth, P.S.L.;Borgland, A.W.;Borisov, G.;Bosio, C.;Botner, O.;Boudinov, E.;Bouquet, B.;Bourdarios, C.;Bowcock, T.J.V.;Boyko, I.;Bozovic, I.;Bozzo, M.;Branchini, P.;Brenke, T.;Brenner, R.A.;Bruckman, P.;Brunet, J.M.;Bugge, L.;Buran, T.;Burgsmuller, T.;Buschbeck, B.;Buschmann, P.;Cabrera, S.;Caccia, M.;Calvi, M.;Camporesi, T.;Canale, V.;Carena, F.;Carroll, L.;Caso, C.;Castillo Gimenez, M.V.;Cattai, A.;Cavallo, F.R.;Chabaud, V.;Charpentier, P.;Chaussard, L.;Checchia, P.;Chelkov, G.A.;Chierici, R.;Chochula, P.;Chorowicz, V.;Chudoba, J.;Cieslik, K.;Collins, P.;Contri, R.;Cortina, E.;Cosme, G.;Cossutti, F.;Cowell, J.H.;Crawley, H.B.;Crennell, D.;Crepe-Renaudin, Sabine;Crosetti, G.;Cuevas Maestro, J.;Czellar, S.;Davenport, M.;Da Silva, W.;Deghorain, A.;Della Ricca, G.;Delpierre, P.;Demaria, N.;De Angelis, A.;De Boer, W.;De Clercq, C.;De Lotto, B.;De Min, A.;De Paula, L.;Dijkstra, H.;Di Ciaccio, L.;Dolbeau, J.;Doroba, K.;Dracos, M.;Drees, J.;Dris, M.;Duperrin, A.;Durand, J.D.;Eigen, G.;Ekelof, T.;Ekspong, G.;Ellert, M.;Elsing, M.;Engel, J.P.;Erzen, B.;Espirito Santo, M.C.;Fanourakis, G.;Fassouliotis, D.;Fayot, J.;Feindt, M.;Ferrari, P.;Ferrer, A.;Ferrer-Ribas, E.;Ferro, F.;Fichet, S.;Firestone, A.;Flagmeyer, U.;Foeth, H.;Fokitis, E.;Fontanelli, F.;Franek, B.;Frodesen, A.G.;Fruhwirth, R.;Fulda-Quenzer, F.;Fuster, J.;Galloni, A.;Gamba, D.;Gamblin, S.;Gandelman, M.;Garcia, C.;Gaspar, C.;Gaspar, M.;Gasparini, U.;Gavillet, P.;Gazis, Evangelos;Gele, D.;Ghodbane, N.;Gil Botella, Ines;Glege, F.;Gokieli, R.;Golob, B.;Gomez-Ceballos, G.;Goncalves, P.;Gonzalez Caballero, I.;Gopal, G.;Gorn, L.;Gracco, V.;Grahl, J.;Graziani, E.;Green, C.;Grimm, H.J.;Gris, P.;Grosdidier, G.;Grzelak, K.;Gunther, M.;Guy, J.;Hahn, F.;Hahn, S.;Haider, S.;Hallgren, A.;Hamacher, K.;Hansen, J.;Harris, F.J.;Hedberg, V.;Heising, S.;Hernandez, J.J.;Herquet, P.;Herr, H.;Hessing, T.L.;Heuser, J.M.;Higon, E.;Holmgren, S.O.;Holt, P.J.;Hoorelbeke, S.;Houlden, M.;Hrubec, J.;Huet, K.;Hughes, G.J.;Hultqvist, K.;Jackson, John Neil;Jacobsson, R.;Jalocha, P.;Janik, R.;Jarlskog, C.;Jarlskog, G.;Jarry, P.;Jean-Marie, B.;Johansson, Erik Karl;Jonsson, P.;Joram, C.;Juillot, P.;Kapusta, Frederic;Karafasoulis, K.;Katsanevas, S.;Katsoufis, E.C.;Keranen, R.;Kersevan, B.P.;Khomenko, B.A.;Khovansky, N.N.;Kiiskinen, A.;King, B.;Kinvig, A.;Kjaer, N.J.;Klapp, O.;Klein, Hansjorg;Kluit, P.;Kokkinias, P.;Koratzinos, M.;Kourkoumelis, C.;Kuznetsov, O.;Krammer, M.;Kriznic, E.;Krumshtein, Z.;Kubinec, P.;Kurowska, J.;Kurvinen, K.;Lamsa, J.W.;Lane, D.W.;Langefeld, P.;Laugier, J.P.;Lauhakangas, R.;Leder, G.;Ledroit, Fabienne;Lefebure, V.;Leinonen, L.;Leisos, A.;Leitner, R.;Lemonne, J.;Lenzen, G.;Lepeltier, V.;Lesiak, T.;Lethuillier, M.;Libby, J.;Liko, D.;Lipniacka, A.;Lippi, I.;Lorstad, B.;Loken, J.G.;Lopes, J.H.;Lopez, J.M.;Lopez-Fernandez, R.;Loukas, D.;Lutz, P.;Lyons, L.;MacNaughton, J.;Mahon, J.R.;Maio, A.;Malek, A.;Malmgren, T.G.M.;Maltezos, S.;Malychev, V.;Mandl, F.;Marco, J.;Marco, R.;Marechal, B.;Margoni, M.;Marin, J.C.;Mariotti, C.;Markou, A.;Martinez-Rivero, C.;Martinez-Vidal, F.;Marti I Garcia, S.;Masik, J.;Mastroyiannopoulos, N.;Matorras, F.;Matteuzzi, C.;Matthiae, G.;Mazzucato, F.;Mazzucato, M.;McCubbin, M.;McKay, R.;McNulty, R.;McPherson, G.;Meroni, C.;Meyer, W.T.;Migliore, E.;Mirabito, L.;Mitaroff, W.A.;Mjornmark, U.;Moa, T.;Moch, M.;Moller, Rasmus;Monig, Klaus;Monge, M.R.;Moreau, X.;Morettini, P.;Morton, G.;Muller, U.;Munich, K.;Mulders, M.;Mulet-Marquis, C.;Muresan, R.;Murray, W.J.;Muryn, B.;Myatt, G.;Myklebust, T.;Naraghi, F.;Nassiakou, M.;Navarria, F.L.;Navas, Sergio;Nawrocki, K.;Negri, P.;Nemecek, S.;Neufeld, N.;Nicolaidou, R.;Nielsen, B.S.;Niezurawski, P.;Nikolenko, M.;Nomokonov, V.;Normand, A.;Nygren, A.;Olshevsky, A.G.;Onofre, A.;Orava, R.;Orazi, G.;Osterberg, K.;Ouraou, A.;Paganoni, M.;Paiano, S.;Pain, R.;Paiva, R.;Palacios, J.;Palka, H.;Papadopoulou, T.D.;Papageorgiou, K.;Pape, L.;Parkes, C.;Parodi, F.;Parzefall, U.;Passeri, A.;Passon, O.;Pegoraro, M.;Peralta, L.;Pernicka, M.;Perrotta, A.;Petridou, C.;Petrolini, A.;Piotto, E.;Podobnik, T.;Pol, M.E.;Polok, G.;Poropat, P.;Pozdnyakov, V.;Privitera, P.;Pukhaeva, N.;Pullia, A.;Radojicic, D.;Ragazzi, S.;Rahmani, H.;Ratoff, P.N.;Read, Alexander L.;Rebecchi, P.;Redaelli, Nicola Giuseppe;Regler, M.;Reid, D.;Reinhardt, R.;Renton, P.B.;Resvanis, L.K.;Richard, F.;Ridky, J.;Rinaudo, G.;Rodrigo, German;Rohne, O.;Romero, A.;Ronchese, P.;Rosenberg, E.I.;Rosinsky, P.;Roudeau, P.;Rovelli, T.;Royon, C.;Ruhlmann-Kleider, V.;Ruiz, A.;Saarikko, H.;Sacquin, Y.;Sadovsky, A.;Sajot, G.;Salt, J.;Sampsonidis, D.;Sannino, M.;Schneider, H.;Schwemling, P.;Schwering, B.;Schwickerath, U.;Schyns, M.A.E.;Scuri, Fabrizio;Seager, P.;Sedykh, Yu.;Segar, A.M.;Sekulin, R.;Shellard, R.C.;Sheridan, A.;Siebel, M.;Simard, L.;Simonetto, F.;Sisakian, A.N.;Smadja, G.;Smirnova, O.;Smith, G.R.;Sopczak, A.;Sosnowski, R.;Spassoff, T.;Spiriti, E.;Sponholz, P.;Squarcia, S.;Stanescu, C.;Stanic, S.;Stevenson, K.;Stocchi, A.;Strauss, J.;Strub, R.;Stugu, B.;Szczekowski, M.;Szeptycka, M.;Tabarelli, T.;Tegenfeldt, F.;Terranova, F.;Thomas, J.;Timmermans, Jan;Tinti, N.;Tkachev, L.G.;Todorova, S.;Tomaradze, A.;Tome, B.;Tonazzo, A.;Tortora, L.;Transtromer, G.;Treille, D.;Tristram, G.;Trochimczuk, M.;Troncon, C.;Tsirou, A.;Turluer, M.L.;Tyapkin, I.A.;Tzamarias, S.;Ullaland, O.;Valenti, G.;Vallazza, E.;Vander Velde, C.;Van Apeldoorn, G.W.;Van Dam, Piet;Van Doninck, Walter;Van Eldik, J.;Van Lysebetten, A.;Van Remortel, N.;Van Vulpen, I.;Vassilopoulos, N.;Vegni, G.;Ventura, L.;Venus, W.;Verbeure, F.;Verlato, M.;Vertogradov, L.S.;Verzi, V.;Vilanova, D.;Vitale, L.;Vodopianov, A.S.;Vollmer, C.;Voulgaris, G.;Vrba, V.;Wahlen, H.;Walck, C.;Weiser, C.;Wicke, D.;Wickens, J.H.;Wilkinson, G.R.;Winter, M.;Witek, M.;Wolf, G.;Yi, J.;Zalewska, A.;Zalewski, P.;Zavrtanik, D.;Zevgolatakos, E.;Zimine, N.I.;Zucchelli, G.C.;Zumerle, G.

Description

CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the final ALPHA-S values together with the event shape distributions integrated over all THETA.CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the Energy Energy Correlation and it Asymmetry and the JetCone Enegy Fraction in 8 ranges of THETA.CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the normalized event shape distributions in 8 THETA ranges.CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the differential two jet rates in a variety of different jet schemes, as a function of the jet separation parameter YCUT, in 8 THETA ranges.

Citations (0)

Mentions (0)

Metrics

Dataset Index

0.1

FAIR Score

15%

Citations

0

Mentions

0

Metrics Over Time

Publication Details

DOI

10.17182/hepdata.12627.v1/t67

Publisher

Eur.Phys.J. C14 (2000) 557-584

Assigned Domain

Subfield

Electrical and Electronic Engineering

Field

Engineering

Domain

Physical Sciences

Confidence Score

37%

Source

Scholar Data Model

Keywords

E+ E- --> CHARGED XE+ E- --> HADRONSE+ E- --> JETSE+ E- --> Z0D2InclusiveExclusiveJet ProductionE+ E- Scattering91.2

Normalization Factors

FT

57.69

CTw

1.00

MTw

1.00