Difference between revisions of "Hadronization"

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[[Category:QCD]]
 
'''Hadronization''' or '''hadron formation''' is the process by which [[Parton|partons]] ([[Quark|quarks]] and [[Gluon|gluons]]), which have [[Color charge|color charge]], form [[Bound state|bound states]] called [[Hadron|hadrons]], which are colorless. Hadronization happens in a [[Nonperturbative QCD|regime]] where the [[strong interaction]] is [[Strong coupling|too strong]] to make calculations using [[Perturbation theory|perturbation theory]]. It can therefore not be [[Ab-initio calculation|calculated from first principles]], but has to be described by a [[phenomenological model]]. Examples of [[Hadronization model|hadronization models]] are the early [[Field-Feynman model]] and the more modern [[Lund string model]] as well as the [[cluster model]].
 
'''Hadronization''' or '''hadron formation''' is the process by which [[Parton|partons]] ([[Quark|quarks]] and [[Gluon|gluons]]), which have [[Color charge|color charge]], form [[Bound state|bound states]] called [[Hadron|hadrons]], which are colorless. Hadronization happens in a [[Nonperturbative QCD|regime]] where the [[strong interaction]] is [[Strong coupling|too strong]] to make calculations using [[Perturbation theory|perturbation theory]]. It can therefore not be [[Ab-initio calculation|calculated from first principles]], but has to be described by a [[phenomenological model]]. Examples of [[Hadronization model|hadronization models]] are the early [[Field-Feynman model]] and the more modern [[Lund string model]] as well as the [[cluster model]].

Revision as of 16:21, 29 November 2016

Hadronization or hadron formation is the process by which partons (quarks and gluons), which have color charge, form bound states called hadrons, which are colorless. Hadronization happens in a regime where the strong interaction is too strong to make calculations using perturbation theory. It can therefore not be calculated from first principles, but has to be described by a phenomenological model. Examples of hadronization models are the early Field-Feynman model and the more modern Lund string model as well as the cluster model.