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1971
Our first observation was that our bootstrap condition implied, for the scattering of S U (3) q¯q-compounds, a degeneracy of the exchange degenerate q - f, ω - A2 trajectories. This conclusion holds for a large variety of dynamical models and remained to hold when S U (3) was broken.
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Our first observation was that our bootstrap condition implied, for the scattering of S U (3) q¯q-compounds, a degeneracy of the exchange degenerate q - f, ω - A2 trajectories. This conclusion holds for a large variety of dynamical models and remained to hold when S U (3) was broken.
openaire +1 more source
Single top-quark production at the Tevatron and the LHC
Reviews of Modern Physics, 2018Andrea Giammanco
exaly
Tetra- and Penta-Quark Structures in the Constituent Quark Model
Symmetry, 2020Gang Yang, Jia-Lun Ping, Jorge Segovia
exaly
The nucleon-nucleon force and the quark degrees of freedom
Reviews of Modern Physics, 1988Fred Myhrer
exaly
Masses of doubly heavy-quark baryons in an extended chromomagnetic model
Physical Review D, 2018Xinzhen Weng, Wei-Zhen Deng
exaly
Strongly coupled quark-gluon plasma in heavy ion collisions
Reviews of Modern Physics, 2017Edward Shuryak
exaly