2019-04-02T11:31:29Z
2019-04-02T11:31:29Z
2014-07-09
2019-04-02T11:31:29Z
The resonant structure of the reaction ¯ B 0 → J / ψ π + π − is studied using data from 3 fb − 1 of integrated luminosity collected by the LHCb experiment, one third at 7 TeV center-of-mass energy and the remainder at 8 TeV. The invariant mass of the π + π − pair and three decay angular distributions are used to determine the fractions of the resonant and nonresonant components. Six interfering π + π − states, ρ ( 770 ) , f 0 ( 500 ) , f 2 ( 1270 ) , ρ ( 1450 ) , ω ( 782 ) and ρ ( 1700 ) , are required to give a good description of invariant mass spectra and decay angular distributions. The positive and negative charge parity fractions of each of the resonant final states are determined. The f 0 ( 980 ) meson is not seen and the upper limit on its presence, compared with the observed f 0 ( 500 ) rate, is inconsistent with a model where these scalar mesons are formed from two quarks and two antiquarks (tetraquarks) at the eight standard deviation level. In the q ¯ q model, the absolute value of the mixing angle between the f 0 ( 980 ) and the f 0 ( 500 ) scalar mesons is limited to be less than 17° at 90% confidence level.
Article
Published version
English
Física de partícules; Gran Col·lisionador d'Hadrons; Ressonància; Experiments; Particle physics; Large Hadron Collider (France and Switzerland); Resonance; Experiments
American Physical Society
Reproducció del document publicat a: https://doi.org/10.1103/PhysRevD.90.012003
Physical Review D, 2014, vol. 90, num. 1, p. 012003
https://doi.org/10.1103/PhysRevD.90.012003
cc by (c) CERN; LHCb Collaboration, 2014
http://creativecommons.org/licenses/by/3.0/es/