Jet Like Distributions From the Weak Decay of Heavy Quarks

Autor: Ali, Ahmed, Korner, J. G., Kramer, G., Willrodt, J.
Jazyk: angličtina
Rok vydání: 1978
Předmět:
BEAUTY MESON [POSTULATED PARTICLE]
PAIR PRODUCTION [QUARK]
QUARK: DECAY
High Energy Physics::Lattice
Nuclear Theory
ENERGY DEPENDENCE
TRANSVERSE MOMENTUM: JET
NONLEPTONIC DECAY: BEAUTY MESON
WEAK INTERACTION [DECAY]
BEAUTY MESON [LEPTONIC DECAY]
DECAY [QUARK]
GAUGE FIELD THEORY: SU(2) X U(1)
(2JET) [FINAL STATE]
(3JET) [FINAL STATE]
LIFETIME: BEAUTY MESON
JET [MODEL]
LEPTONIC DECAY: BEAUTY MESON
SU(2) X U(1) [GAUGE FIELD THEORY]
JET [TRANSVERSE MOMENTUM]
ddc:530
BEAUTY MESON [NONLEPTONIC DECAY]
heavy quark
DECAY WIDTH [RATIO]
POSTULATED PARTICLE: BEAUTY MESON
DIFFERENTIAL CROSS SECTION: SPHERICITY
BEAUTY MESON [SEMILEPTONIC DECAY]
High Energy Physics::Phenomenology
SPHERICITY [DIFFERENTIAL CROSS SECTION]
FINAL STATE: (3JET)
DIFFERENTIAL CROSS SECTION: THRUST
UP TO 200 GEV-CM
BEAUTY MESON [LIFETIME]
PAIR PRODUCTION: QUARK
ANNIHILATION: ELECTRON POSITRON
QUARK [DECAY]
THRUST [DIFFERENTIAL CROSS SECTION]
SEMILEPTONIC DECAY: BEAUTY MESON
ELECTRON POSITRON [ANNIHILATION]
MODEL: JET
FINAL STATE: (2JET)
RATIO: DECAY WIDTH
ANNIHILATION [ELECTRON POSITRON]
DECAY: QUARK
QUARK [PAIR PRODUCTION]
High Energy Physics::Experiment
QUARK: PAIR PRODUCTION
ELECTRON POSITRON: ANNIHILATION
DECAY: WEAK INTERACTION
Zdroj: (1979). doi:10.1007/BF01445412
DOI: 10.3204/pubdb-2017-12716
Popis: (1979). doi:10.1007/BF01445412
We consider the production and weak decay of a pair of heavy quarks (mesons) ine+e− experiments and study their effect on the various jet distributions. The relative magnitudes of the two-quark-jet and three-quark-jet final states, in the decay of a heavy quark are estimated in the framework of an SU(2)L×U(1) model. We find that the three quark configuration dominates over the two quark configuration. For the quark jets resulting from the weak decay of the heavy quarks, we calculate the jet distributions in Sphericity, Spherocity and Thrust for the process\(e^ +e^ -\to Q\bar Q \to 6\) quarks. These distributions are compared with the corresponding quantities from the non-perturbative process\(e^ +e^ -\to q\bar q\) and the QCD process\(e^ +e^ -\to q\bar qg\). We find that the weak decay of heavy quarks is the dominant mechanism for jet broadening ine+e− experiments, in the intermediate energy region relevant for PETRA and PEP.
Databáze: OpenAIRE