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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...
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Lenguaje: | eng |
Publicado: |
2006
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Acceso en línea: | https://dx.doi.org/10.1016/j.physletb.2006.10.071 http://cds.cern.ch/record/1047414 |
_version_ | 1780912803870146560 |
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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 |