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Oxana Smirnova

Oxana Smirnova

Senior Lecturer, Deputy Head of division

Oxana Smirnova

A study of the energy evolution of event shape distributions and their means with the DELPHI detector at LEP

Author

  • J Abdallah
  • P Abreu
  • W Adam
  • P Adzic
  • T Albrecht
  • T Alderweireld
  • R Alemany-Fernandez
  • T Allmendinger
  • PP Allport
  • U Amaldi
  • N Amapane
  • S Amato
  • E Anashkin
  • A Andreazza
  • S Andringa
  • N Anjos
  • P Antilogus
  • WD Apel
  • Y Arnoud
  • Stefan Ask
  • B Asman
  • JE Augustin
  • A Augustinus
  • P Baillon
  • A Ballestrero
  • P Bambade
  • R Barbier
  • D Bardin
  • G Barker
  • A Baroncelli
  • M Battaglia
  • M Baubillier
  • KH Becks
  • M Begalli
  • A Behrmann
  • E Ben-Haim
  • N Benekos
  • A Benvenuti
  • C Berat
  • M Berggren
  • L Berntzon
  • D Bertrand
  • M Besancon
  • N Besson
  • D Bloch
  • M Blom
  • M Bluj
  • M Bonesini
  • M Boonekamp
  • PSL Booth
  • G Borisov
  • O Botner
  • B Bouquet
  • TJV Bowcock
  • I Boyko
  • M Bracko
  • R Brenner
  • E Brodet
  • P Bruckman
  • JM Brunet
  • L Bugge
  • P Buschmann
  • M Calvi
  • T Camporesi
  • V Canale
  • F Carena
  • N Castro
  • F Cavallo
  • M Chapkin
  • P Charpentier
  • P Checchia
  • R Chierici
  • P Chliapnikov
  • J Chudoba
  • SU Chung
  • K Cieslik
  • P Collins
  • R Contri
  • G Cosme
  • F Cossutti
  • MJ Costa
  • B Crawley
  • D Crennell
  • J Cuevas
  • J D'Hondt
  • J Dalmau
  • T da Silva
  • W Da Silva
  • G Della Ricca
  • A De Angelis
  • W De Boer
  • C De Clercq
  • B De Lotto
  • N De Maria
  • A De Min
  • L de Paula
  • L Di Ciaccio
  • A Di Simone
  • K Doroba
  • J Drees
  • M Dris
  • G Eigen
  • T Ekelof
  • M Ellert
  • M Elsing
  • MCE Santo
  • G Fanourakis
  • D Fassouliotis
  • M Feindt
  • J Fernandez
  • A Ferrer
  • F Ferro
  • U Flagmeyer
  • H Foeth
  • E Fokitis
  • F Fulda-Quenzer
  • J Fuster
  • M Gandelman
  • C Garcia
  • P Gavillet
  • E Gazis
  • R Gokieli
  • B Golob
  • G Gomez-Ceballos
  • P Goncalves
  • E Graziani
  • G Grosdidier
  • K Grzelak
  • J Guy
  • C Haag
  • A Hallgren
  • K Hamacher
  • K Hamilton
  • J Hansen
  • S Haug
  • F Hauler
  • Vincent Hedberg
  • M Hennecke
  • H Herr
  • J Hoffman
  • SO Holmgren
  • PJ Holt
  • MA Houlden
  • K Hultqvist
  • JN Jackson
  • Göran Jarlskog
  • P Jarry
  • D Jeans
  • EK Johansson
  • PD Johansson
  • P Jonsson
  • C Joram
  • L Jungermann
  • F Kapusta
  • S Katsanevas
  • E Katsoufis
  • G Kernel
  • BP Kersevan
  • A Kiiskinen
  • BT King
  • NJ Kjaer
  • P Kluit
  • P Kokkinias
  • C Kourkoumelis
  • O Kouznetsov
  • Z Krumstein
  • M Kucharczyk
  • J Lamsa
  • G Leder
  • F Ledroit
  • L Leinonen
  • R Leitner
  • J Lemonne
  • V Lepeltier
  • T Lesiak
  • W Liebig
  • D Liko
  • A Lipniacka
  • JH Lopes
  • JM Lopez
  • D Loukas
  • P Lutz
  • L Lyons
  • J MacNaughton
  • A Malek
  • S Maltezos
  • F Mandl
  • J Marco
  • R Marco
  • B Marechal
  • M Margoni
  • JC Marin
  • C Mariotti
  • A Markou
  • C Martinez-Rivero
  • J Masik
  • N Mastroyiannopoulos
  • F Matorras
  • C Matteuzzi
  • F Mazzucato
  • M Mazzucato
  • R Mc Nulty
  • C Meroni
  • WT Meyer
  • E Migliore
  • W Mitaroff
  • Ulf Mjörnmark
  • T Moa
  • M Moch
  • K Moenig
  • R Monge
  • J Montenegro
  • D Moraes
  • S Moreno
  • P Morettini
  • U Mueller
  • K Muenich
  • M Mulders
  • L Mundim
  • W Murray
  • B Muryn
  • G Myatt
  • T Myklebust
  • M Nassiakou
  • F Navarria
  • K Nawrocki
  • R Nicolaidou
  • M Nikolenko
  • A Oblakowska-Mucha
  • V Obraztsov
  • A Olshevski
  • A Onofre
  • R Orava
  • K Osterberg
  • A Ouraou
  • A Oyanguren
  • M Paganoni
  • S Paiano
  • JP Palacios
  • H Palka
  • TD Papadopoulou
  • L Pape
  • C Parkes
  • F Parodi
  • U Parzefall
  • A Passeri
  • O Passon
  • L Peralta
  • V Perepelitsa
  • A Perrotta
  • A Petrolini
  • J Piedra
  • L Pieri
  • F Pierre
  • M Pimenta
  • E Piotto
  • T Podobnik
  • V Poireau
  • ME Pol
  • G Polok
  • P Poropat
  • V Pozdniakov
  • N Pukhaeva
  • A Pullia
  • J Rames
  • L Ramler
  • A Read
  • P Rebecchi
  • J Rehn
  • D Reid
  • R Reinhardt
  • P Renton
  • F Richard
  • J Ridky
  • M Rivero
  • D Rodriguez
  • A Romero
  • P Ronchese
  • E Rosenberg
  • P Roudeau
  • T Rovelli
  • V Ruhlmann-Kleider
  • D Ryabtchikov
  • A Sadovsky
  • L Salmi
  • J Salt
  • A Savoy-Navarro
  • U Schwickerath
  • A Segar
  • R Sekulin
  • M Siebel
  • A Sisakian
  • G Smadja
  • Oxana Smirnova
  • A Sokolov
  • A Sopczak
  • R Sosnowski
  • T Spassov
  • M Stanitzki
  • A Stocchi
  • J Strauss
  • B Stugu
  • M Szczekowski
  • M Szeptycka
  • T Szumlak
  • T Tabarelli
  • AC Taffard
  • F Tegenfeldt
  • J Timmermans
  • L Tkatchev
  • M Tobin
  • S Todorovova
  • B Tome
  • A Tonazzo
  • P Tortosa
  • P Travnicek
  • D Treille
  • G Tristram
  • M Trochimczuk
  • C Troncon
  • ML Turluer
  • IA Tyapkin
  • P Tyapkin
  • S Tzamarias
  • V Uvarov
  • G Valenti
  • P Van Dam
  • J Van Eldik
  • A Van Lysebetten
  • N van Remortel
  • I Van Vulpen
  • G Vegni
  • F Veloso
  • W Venus
  • F Verbeure
  • P Verdier
  • V Verzi
  • D Vilanova
  • L Vitale
  • V Vrba
  • H Wahlen
  • AJ Washbrook
  • C Weiser
  • D Wicke
  • J Wickens
  • G Wilkinson
  • M Winter
  • M Witek
  • O Yushchenko
  • A Zalewska
  • P Zalewski
  • D Zavrtanik
  • V Zhuravlov
  • NI Zimin
  • A Zintchenko
  • M Zupan

Summary, in English

Infrared and collinear safe event shape distributions and their mean values are determined in e(+)e(-) collisions at centre-of-mass energies between 45 and 202GeV. A phenomenological analysis based on power correction models including hadron mass effects for both differential distributions and mean values is presented. Using power corrections, alpha(s) is extracted from the mean values and shapes. In an alternative approach, renormalisation group invariance (RGI) is used as an explicit constraint, leading to a consistent description of mean values without the need for sizeable power corrections. The QCD beta-function is precisely measured using this approach. From the DELPHI data on Thrust, including data from low energy experiments, one finds beta(0) = 7.86 +/- 0.32 for the one loop coefficient of the beta-function or, assuming QCD, n(f) = 4.75 +/- 0.44 for the number of active flavours. These values agree well with the QCD expectation of beta(0) = 7.67 and n(f) 5. A direct measurement of the full logarithmic energy slope excludes light gluinos with a mass below 5GeV.

Department/s

  • Particle and nuclear physics

Publishing year

2003

Language

English

Pages

285-312

Publication/Series

European Physical Journal C. Particles and Fields

Volume

29

Issue

3

Document type

Journal article

Publisher

Springer

Topic

  • Subatomic Physics

Status

Published

ISBN/ISSN/Other

  • ISSN: 1434-6044