First measurement of the charge asymmetry in beauty-quark pair production.

نویسندگان

  • R Aaij
  • B Adeva
  • M Adinolfi
  • A Affolder
  • Z Ajaltouni
  • S Akar
  • J Albrecht
  • F Alessio
  • M Alexander
  • S Ali
  • G Alkhazov
  • P Alvarez Cartelle
  • A A Alves
  • S Amato
  • S Amerio
  • Y Amhis
  • L An
  • L Anderlini
  • J Anderson
  • R Andreassen
  • M Andreotti
  • J E Andrews
  • R B Appleby
  • O Aquines Gutierrez
  • F Archilli
  • A Artamonov
  • M Artuso
  • E Aslanides
  • G Auriemma
  • M Baalouch
  • S Bachmann
  • J J Back
  • A Badalov
  • V Balagura
  • W Baldini
  • R J Barlow
  • C Barschel
  • S Barsuk
  • W Barter
  • V Batozskaya
  • V Battista
  • A Bay
  • L Beaucourt
  • J Beddow
  • F Bedeschi
  • I Bediaga
  • S Belogurov
  • K Belous
  • I Belyaev
  • E Ben-Haim
  • G Bencivenni
  • S Benson
  • J Benton
  • A Berezhnoy
  • R Bernet
  • M-O Bettler
  • M van Beuzekom
  • A Bien
  • S Bifani
  • T Bird
  • A Bizzeti
  • P M Bjørnstad
  • T Blake
  • F Blanc
  • J Blouw
  • S Blusk
  • V Bocci
  • A Bondar
  • N Bondar
  • W Bonivento
  • S Borghi
  • A Borgia
  • M Borsato
  • T J V Bowcock
  • E Bowen
  • C Bozzi
  • T Brambach
  • J van den Brand
  • J Bressieux
  • D Brett
  • M Britsch
  • T Britton
  • J Brodzicka
  • N H Brook
  • H Brown
  • A Bursche
  • G Busetto
  • J Buytaert
  • S Cadeddu
  • R Calabrese
  • M Calvi
  • M Calvo Gomez
  • A Camboni
  • P Campana
  • D Campora Perez
  • A Carbone
  • G Carboni
  • R Cardinale
  • A Cardini
  • H Carranza-Mejia
  • L Carson
  • K Carvalho Akiba
  • G Casse
  • L Cassina
  • L Castillo Garcia
  • M Cattaneo
  • Ch Cauet
  • R Cenci
  • M Charles
  • Ph Charpentier
  • S Chen
  • S-F Cheung
  • N Chiapolini
  • M Chrzaszcz
  • K Ciba
  • X Cid Vidal
  • G Ciezarek
  • P E L Clarke
  • M Clemencic
  • H V Cliff
  • J Closier
  • V Coco
  • J Cogan
  • E Cogneras
  • P Collins
  • A Comerma-Montells
  • A Contu
  • A Cook
  • M Coombes
  • S Coquereau
  • G Corti
  • M Corvo
  • I Counts
  • B Couturier
  • G A Cowan
  • D C Craik
  • M Cruz Torres
  • S Cunliffe
  • R Currie
  • C D'Ambrosio
  • J Dalseno
  • P David
  • P N Y David
  • A Davis
  • K De Bruyn
  • S De Capua
  • M De Cian
  • J M De Miranda
  • L De Paula
  • W De Silva
  • P De Simone
  • D Decamp
  • M Deckenhoff
  • L Del Buono
  • N Déléage
  • D Derkach
  • O Deschamps
  • F Dettori
  • A Di Canto
  • H Dijkstra
  • S Donleavy
  • F Dordei
  • M Dorigo
  • A Dosil Suárez
  • D Dossett
  • A Dovbnya
  • K Dreimanis
  • G Dujany
  • F Dupertuis
  • P Durante
  • R Dzhelyadin
  • A Dziurda
  • A Dzyuba
  • S Easo
  • U Egede
  • V Egorychev
  • S Eidelman
  • S Eisenhardt
  • U Eitschberger
  • R Ekelhof
  • L Eklund
  • I El Rifai
  • Ch Elsasser
  • S Ely
  • S Esen
  • H-M Evans
  • T Evans
  • A Falabella
  • C Färber
  • C Farinelli
  • N Farley
  • S Farry
  • Rf Fay
  • D Ferguson
  • V Fernandez Albor
  • F Ferreira Rodrigues
  • M Ferro-Luzzi
  • S Filippov
  • M Fiore
  • M Fiorini
  • M Firlej
  • C Fitzpatrick
  • T Fiutowski
  • M Fontana
  • F Fontanelli
  • R Forty
  • O Francisco
  • M Frank
  • C Frei
  • M Frosini
  • J Fu
  • E Furfaro
  • A Gallas Torreira
  • D Galli
  • S Gallorini
  • S Gambetta
  • M Gandelman
  • P Gandini
  • Y Gao
  • J García Pardiñas
  • J Garofoli
  • J Garra Tico
  • L Garrido
  • C Gaspar
  • R Gauld
  • L Gavardi
  • G Gavrilov
  • E Gersabeck
  • M Gersabeck
  • T Gershon
  • Ph Ghez
  • A Gianelle
  • S Giani'
  • V Gibson
  • L Giubega
  • V V Gligorov
  • C Göbel
  • D Golubkov
  • A Golutvin
  • A Gomes
  • H Gordon
  • C Gotti
  • M Grabalosa Gándara
  • R Graciani Diaz
  • L A Granado Cardoso
  • E Graugés
  • G Graziani
  • A Grecu
  • E Greening
  • S Gregson
  • P Griffith
  • L Grillo
  • O Grünberg
  • B Gui
  • E Gushchin
  • Yu Guz
  • T Gys
  • C Hadjivasiliou
  • G Haefeli
  • C Haen
  • S C Haines
  • S Hall
  • B Hamilton
  • T Hampson
  • X Han
  • S Hansmann-Menzemer
  • N Harnew
  • S T Harnew
  • J Harrison
  • J He
  • T Head
  • V Heijne
  • K Hennessy
  • P Henrard
  • L Henry
  • J A Hernando Morata
  • E van Herwijnen
  • M Heß
  • A Hicheur
  • D Hill
  • M Hoballah
  • C Hombach
  • W Hulsbergen
  • P Hunt
  • N Hussain
  • D Hutchcroft
  • D Hynds
  • M Idzik
  • P Ilten
  • R Jacobsson
  • A Jaeger
  • J Jalocha
  • E Jans
  • P Jaton
  • A Jawahery
  • F Jing
  • M John
  • D Johnson
  • C R Jones
  • C Joram
  • B Jost
  • N Jurik
  • M Kaballo
  • S Kandybei
  • W Kanso
  • M Karacson
  • T M Karbach
  • S Karodia
  • M Kelsey
  • I R Kenyon
  • T Ketel
  • B Khanji
  • C Khurewathanakul
  • S Klaver
  • K Klimaszewski
  • O Kochebina
  • M Kolpin
  • I Komarov
  • R F Koopman
  • P Koppenburg
  • M Korolev
  • A Kozlinskiy
  • L Kravchuk
  • K Kreplin
  • M Kreps
  • G Krocker
  • P Krokovny
  • F Kruse
  • W Kucewicz
  • M Kucharczyk
  • V Kudryavtsev
  • K Kurek
  • T Kvaratskheliya
  • V N La Thi
  • D Lacarrere
  • G Lafferty
  • A Lai
  • D Lambert
  • R W Lambert
  • E Lanciotti
  • G Lanfranchi
  • C Langenbruch
  • B Langhans
  • T Latham
  • C Lazzeroni
  • R Le Gac
  • J van Leerdam
  • J-P Lees
  • R Lefèvre
  • A Leflat
  • J Lefrançois
  • S Leo
  • O Leroy
  • T Lesiak
  • B Leverington
  • Y Li
  • M Liles
  • R Lindner
  • C Linn
  • F Lionetto
  • B Liu
  • G Liu
  • S Lohn
  • I Longstaff
  • J H Lopes
  • N Lopez-March
  • P Lowdon
  • H Lu
  • D Lucchesi
  • H Luo
  • A Lupato
  • E Luppi
  • O Lupton
  • F Machefert
  • I V Machikhiliyan
  • F Maciuc
  • O Maev
  • S Malde
  • G Manca
  • G Mancinelli
  • J Maratas
  • J F Marchand
  • U Marconi
  • C Marin Benito
  • P Marino
  • R Märki
  • J Marks
  • G Martellotti
  • A Martens
  • A Martín Sánchez
  • M Martinelli
  • D Martinez Santos
  • F Martinez Vidal
  • D Martins Tostes
  • A Massafferri
  • R Matev
  • Z Mathe
  • C Matteuzzi
  • A Mazurov
  • M McCann
  • J McCarthy
  • A McNab
  • R McNulty
  • B McSkelly
  • B Meadows
  • F Meier
  • M Meissner
  • M Merk
  • D A Milanes
  • M-N Minard
  • N Moggi
  • J Molina Rodriguez
  • S Monteil
  • M Morandin
  • P Morawski
  • A Mordà
  • M J Morello
  • J Moron
  • A-B Morris
  • R Mountain
  • F Muheim
  • K Müller
  • R Muresan
  • M Mussini
  • B Muster
  • P Naik
  • T Nakada
  • R Nandakumar
  • I Nasteva
  • M Needham
  • N Neri
  • S Neubert
  • N Neufeld
  • M Neuner
  • A D Nguyen
  • T D Nguyen
  • C Nguyen-Mau
  • M Nicol
  • V Niess
  • R Niet
  • N Nikitin
  • T Nikodem
  • A Novoselov
  • D P O'Hanlon
  • A Oblakowska-Mucha
  • V Obraztsov
  • S Oggero
  • S Ogilvy
  • O Okhrimenko
  • R Oldeman
  • G Onderwater
  • M Orlandea
  • J M Otalora Goicochea
  • P Owen
  • A Oyanguren
  • B K Pal
  • A Palano
  • F Palombo
  • M Palutan
  • J Panman
  • A Papanestis
  • M Pappagallo
  • C Parkes
  • C J Parkinson
  • G Passaleva
  • G D Patel
  • M Patel
  • C Patrignani
  • A Pazos Alvarez
  • A Pearce
  • A Pellegrino
  • M Pepe Altarelli
  • S Perazzini
  • E Perez Trigo
  • P Perret
  • M Perrin-Terrin
  • L Pescatore
  • E Pesen
  • K Petridis
  • A Petrolini
  • E Picatoste Olloqui
  • B Pietrzyk
  • T Pilař
  • D Pinci
  • A Pistone
  • S Playfer
  • M Plo Casasus
  • F Polci
  • A Poluektov
  • E Polycarpo
  • A Popov
  • D Popov
  • B Popovici
  • C Potterat
  • E Price
  • J Prisciandaro
  • A Pritchard
  • C Prouve
  • V Pugatch
  • A Puig Navarro
چکیده

The difference in the angular distributions between beauty quarks and antiquarks, referred to as the charge asymmetry, is measured for the first time in bb pair production at a hadron collider. The data used correspond to an integrated luminosity of 1.0 fb(-1) collected at 7 TeV center-of-mass energy in proton-proton collisions with the LHCb detector. The measurement is performed in three regions of the invariant mass of the bb system. The results obtained are A(C)(bb))(40 105 GeV/c(2)) = 1.6 ± 1.7 ± 0.6%, where A(C)(bb)) is defined as the asymmetry in the difference in rapidity between jets formed from the beauty quark and antiquark, where in each case the first uncertainty is statistical and the second systematic. The beauty jets are required to satisfy 2 < η < 4, E(T) >20 GeV, and have an opening angle in the transverse plane Δ ϕ > 2.6 rad. These measurements are consistent with the predictions of the standard model.

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Measurement of the Forward-Backward Charge Asymmetry in Top-Quark Pair Production in Proton-Antiproton Collisions at DØ

A measurement of the forward-backward charge asymmetry in top-antitop (tt̄) pair production in proton-antiproton (pp̄) collisions is presented. The asymmetry is measured for different jet multiplicities in the lepton+jets final state on 0.9 fb−1 of data collected by the DØ experiment at the Fermilab Tevatron Collider. The result is sensitive to new physics, which is demonstrated by setting an upp...

متن کامل

Lepton pair production in a charged quark gluon plasma

We investigate the effects of a charge asymmetry on the spectrum of dileptons radiating from a quark gluon plasma. We demonstrate the existence of a new set of processes in this regime. The dilepton production rate from the corresponding diagrams is shown to be as important as that obtained from the Born-term quark-antiquark annihilation.

متن کامل

QCD and Intrinsic Heavy Quark Predictions for Leading Charm and Beauty Hadroproduction

Recent experiments at Fermilab and CERN have observed a strong asymmetry between the hadroproduction cross sections of leading D mesons, containing projectile valence quarks, and nonleading charmed mesons, without projectile valence quarks. The observed correlations of the πN → DX cross section with the projectile charge violates the usual assumption that heavy quark jet fragmentation factorize...

متن کامل

Measurement of the forward-backward charge asymmetry in top quark production in proton-antiproton collisions at 1.96 TeV

We report on the D0 measurement of the top-antitop charge production asymmetry based on 5.4 f b −1 of data. Asymmetry dependence on the invariant mass of the top-antitop system, its transverse momentum, as well as the number of extra jets is discussed.

متن کامل

Measurement of the Forward-Backward Asymmetry in Bottom-Quark Pair Production Using Soft Muon

We investigate the forward-backward asymmetry, AFB, in b-quark pair production in protonantiproton collision at √ s = 1.96 GeV with the CDF detector. The soft muon tag technique has been applied to identify bb̄ production. Using the full CDF data set (6.9 fb−1) we have obtained the integrated asymmetry at particle level of AFB= (1.2 ± 0.7)% for dijet invariant mass above 40 GeV/c. Dependence of ...

متن کامل

Asymmetries in the angular distributions in the tt̄ system

Asymmetries in the pair production of top–antitop quarks in hadronic collisions have gained a lot of attention because the size of the effect exceeded the predictions based on the Standard Model (SM). To understand the basis for these predictions as well as the importance of this measurement and its experimental subtleties, it is instructive to review its historic predecessor — the asymmetry of...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

عنوان ژورنال:
  • Physical review letters

دوره 113 8  شماره 

صفحات  -

تاریخ انتشار 2014