Canonical quantization in temporal gauge produces instantaneous bound-state potentials in QED and QCD; a non-vanishing boundary condition on the longitudinal gluon field at infinity yields confinement for color singlets and permits perturbative hadron calculations plus spontaneous chiral symmetry br
Quarkonia and their transitions
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abstract
Valuable data on quarkonia (the bound states of a heavy quark Q=c,b and the corresponding antiquark) have recently been provided by a variety of sources, mainly e+ e- collisions, but also hadronic interactions. This permits a thorough updating of the experimental and theoretical status of electromagnetic and strong transitions in quarkonia. We discuss QQbar transitions to other QQbar states, with some reference to processes involving QQbar annihilation.
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hep-ph 1years
2026 1verdicts
UNVERDICTED 1representative citing papers
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Principles and Possibilities for Bound States in Gauge Theory
Canonical quantization in temporal gauge produces instantaneous bound-state potentials in QED and QCD; a non-vanishing boundary condition on the longitudinal gluon field at infinity yields confinement for color singlets and permits perturbative hadron calculations plus spontaneous chiral symmetry br