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Mass Generation in QCD -- Oscillating Quarks and Gluons
The present lecture is devoted to embedding the approximate genuine harmonic oscillator structure of valence q qbar mesons and in more detail the q q q configurations for up,down,strange - flavored baryons in Q C D for three light flavors of quark.
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Lenguaje: | eng |
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2014
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Acceso en línea: | https://dx.doi.org/10.1142/S0217751X14440151 http://cds.cern.ch/record/1699142 |
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author | Minkowski, Peter |
author_facet | Minkowski, Peter |
author_sort | Minkowski, Peter |
collection | CERN |
description | The present lecture is devoted to embedding the approximate genuine harmonic oscillator structure of valence q qbar mesons and in more detail the q q q configurations for up,down,strange - flavored baryons in Q C D for three light flavors of quark. |
id | cern-1699142 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2014 |
record_format | invenio |
spelling | cern-16991422021-05-03T20:14:07Zdoi:10.1142/S0217751X14440151http://cds.cern.ch/record/1699142engMinkowski, PeterMass Generation in QCD -- Oscillating Quarks and GluonsParticle Physics - TheoryThe present lecture is devoted to embedding the approximate genuine harmonic oscillator structure of valence q qbar mesons and in more detail the q q q configurations for up,down,strange - flavored baryons in Q C D for three light flavors of quark.The present lecture is devoted to embedding the approximate genuine harmonic oscillator structure of valence $q\bar{q}$ mesons and in more detail the qqq configurations for u, d, s flavored baryons in QCD for three light flavors of quark. It includes notes, preparing the counting of "oscillatory modes of Nfl = 3 light quarks, u, d, s in baryons," using the $SU(2N_{\rm fl} = 6) \times SO3(\vec{L})$ broken symmetry classification, extended to the harmonic oscillator symmetry of 3 paired oscillator modes. $\vec{L} = \sum_{n = 1}{N_{\rm fl}}\vec{L}_{n}$ stands for the space rotation group generated by the sum of the 3 individual angular momenta of quarks in their c.m. system. The oscillator extension to valence gauge boson states is not yet developed to a comparable level.The present lecture is devoted to embedding the approximate genuine harmonic oscillator structure of valence q qbar mesons and in more detail the q q q configurations for up,down,strange - flavored baryons in Q C D for three light flavors of quark.The present lecture is devoted to embedding the approximate genuine harmonic oscillator structure of valence $q\bar{q}$ mesons and in more detail the qqq configurations for u, d, s flavored baryons in QCD for three light flavors of quark. It includes notes, preparing the counting of "oscillatory modes of Nfl = 3 light quarks, u, d, s in baryons," using the $SU(2N_{\rm fl} = 6) \times SO3(\vec{L})$ broken symmetry classification, extended to the harmonic oscillator symmetry of 3 paired oscillator modes. $\vec{L} = \sum_{n = 1}^{N_{\rm fl}}\vec{L}_{n}$ stands for the space rotation group generated by the sum of the 3 individual angular momenta of quarks in their c.m. system. The oscillator extension to valence gauge boson states is not yet developed to a comparable level.arXiv:1404.5052oai:cds.cern.ch:16991422014-04-20 |
spellingShingle | Particle Physics - Theory Minkowski, Peter Mass Generation in QCD -- Oscillating Quarks and Gluons |
title | Mass Generation in QCD -- Oscillating Quarks and Gluons |
title_full | Mass Generation in QCD -- Oscillating Quarks and Gluons |
title_fullStr | Mass Generation in QCD -- Oscillating Quarks and Gluons |
title_full_unstemmed | Mass Generation in QCD -- Oscillating Quarks and Gluons |
title_short | Mass Generation in QCD -- Oscillating Quarks and Gluons |
title_sort | mass generation in qcd -- oscillating quarks and gluons |
topic | Particle Physics - Theory |
url | https://dx.doi.org/10.1142/S0217751X14440151 http://cds.cern.ch/record/1699142 |
work_keys_str_mv | AT minkowskipeter massgenerationinqcdoscillatingquarksandgluons |