T-2, Nuclear and Particle Physics, Astrophysics and Cosmology

Oscillatory modes of quarks in baryons for 3 quark flavors u , d , s

Peter Minkowski
Albert Einstein Center for Fundamental Physics - ITP, University of Bern

The present outline shall illustrate new features of 'oscillatory modes of Nfl = 3 light quarks', –u,d,s–, using the SU( 2 N fl = 6) × SO3 (L⃗) broken symmetry classification. L⃗ = Sum_{n=1}^Nfl L⃗n 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.

NNSA


Contact Us | Careers | Bradbury Science Museum | Emergencies | Inside LANL | Maps | Site Feedback | SSL Portal | Training

Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA© Copyright 2010-11 LANS, LLC All rights reserved | Terms of Use | Privacy Policy