Chapter

Strings in the Yang-Mills Theory: How They Form, Live and Decay

DOI: 10.1007/3-540-26798-0_39
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    ABSTRACT: The present notes prepare the counting of 'oscillatory modes of N-fl = 3 light quarks', - u, d, s -, using the SU (2 N-fl = 6 ) x SO3 ((L) over right arrow) broken symmetry classification, extended to the harmonic oscillator symmetry of 3 paired oscillator modes. (L) over right arrow = Sigma (n) (=) (1) (Nfl) (L) over right arrow (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 motivation arises from modeling the yields of hadrons in heavy ion collisions at RHIC and LHC, necessitating at the respective highest c. m. energies per nucleon pairs an increase of heavy hadron resonances relative to e. g. SPS energies, whence the included hadrons are treated as a noninteracting gas
    No preview · Conference Paper · Aug 2013
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    ABSTRACT: The present lecture is devoted to embedding the approximate genuine harmonic oscillator structure of valence 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 broken symmetry classification, extended to the harmonic oscillator symmetry of 3 paired oscillator modes. 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.
    Full-text · Article · Apr 2014 · International Journal of Modern Physics A