Cargando…

Is the fragmentation of charm quarks into D mesons described by heavy quark effective theory?

Heavy quark effective theory predicts that produced charm quarks have the same probability to fragment into any of the four D mesons with orbital angular momentum L=0: the singlet D state and the triplet D* states. This would imply PV(D*,D)=3/4, where PV is the ratio between directly produced L=0 ve...

Descripción completa

Detalles Bibliográficos
Autor principal: David, André
Lenguaje:eng
Publicado: 2006
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2006.10.071
http://cds.cern.ch/record/1047414
_version_ 1780912803870146560
author David, André
author_facet David, André
author_sort David, André
collection CERN
description Heavy quark effective theory predicts that produced charm quarks have the same probability to fragment into any of the four D mesons with orbital angular momentum L=0: the singlet D state and the triplet D* states. This would imply PV(D*,D)=3/4, where PV is the ratio between directly produced L=0 vector states (D*) and all L=0 (D and D*) states. Experimental data collected in several different collision systems (e+e-, hadro-production, photo-production, etc.) and over a broad range of collision energies, show that PV(D*,D)=0.594+-0.010. From this observation, it follows that "naive spin counting" does not apply to charm production, implying a revision of charm production calculations where this assumption is made.
id cern-1047414
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2006
record_format invenio
spelling cern-10474142019-09-30T06:29:59Zdoi:10.1016/j.physletb.2006.10.071http://cds.cern.ch/record/1047414engDavid, AndréIs the fragmentation of charm quarks into D mesons described by heavy quark effective theory?Particle Physics - ExperimentParticle Physics - PhenomenologyHeavy quark effective theory predicts that produced charm quarks have the same probability to fragment into any of the four D mesons with orbital angular momentum L=0: the singlet D state and the triplet D* states. This would imply PV(D*,D)=3/4, where PV is the ratio between directly produced L=0 vector states (D*) and all L=0 (D and D*) states. Experimental data collected in several different collision systems (e+e-, hadro-production, photo-production, etc.) and over a broad range of collision energies, show that PV(D*,D)=0.594+-0.010. From this observation, it follows that "naive spin counting" does not apply to charm production, implying a revision of charm production calculations where this assumption is made.CERN-PH-EP-2006-027oai:cds.cern.ch:10474142006-08-06
spellingShingle Particle Physics - Experiment
Particle Physics - Phenomenology
David, André
Is the fragmentation of charm quarks into D mesons described by heavy quark effective theory?
title Is the fragmentation of charm quarks into D mesons described by heavy quark effective theory?
title_full Is the fragmentation of charm quarks into D mesons described by heavy quark effective theory?
title_fullStr Is the fragmentation of charm quarks into D mesons described by heavy quark effective theory?
title_full_unstemmed Is the fragmentation of charm quarks into D mesons described by heavy quark effective theory?
title_short Is the fragmentation of charm quarks into D mesons described by heavy quark effective theory?
title_sort is the fragmentation of charm quarks into d mesons described by heavy quark effective theory?
topic Particle Physics - Experiment
Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.physletb.2006.10.071
http://cds.cern.ch/record/1047414
work_keys_str_mv AT davidandre isthefragmentationofcharmquarksintodmesonsdescribedbyheavyquarkeffectivetheory