QCD forces and heavy quark bound states
By Gunnar S. Bali. 2000
493 citations recorded by the source corpus.
Abstract The present knowledge of QCD confining forces between static test charges is summarised, with an emphasis on lattice results. Recent developments in relating QCD potentials to quarkonium properties by use of effective field theory methods are presented. The validity of non-relativistic QCD and the adiabatic approximation with respect to heavy quark bound states is explored. Besides the static potential and relativistic correction terms, the spectra of glueballs and gluinoballs, hybrid excitations of the QCD flux tube between fundamental colour sources, potentials between charges in various representations of the SU (3) gauge group, and multi-particle interactions are discussed. Some implications for quarkonia systems and quark–gluon hybrid mesons are drawn.
Subfields: Atomic and Molecular Physics, and Optics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/b56e6bd99e122e998e6e9afe61877daa530184c9
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In Atomic and Molecular Physics, and Optics
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In Nuclear and High Energy Physics
Citations in the corpus
- Effective field theories for heavy quarkonium (2004, methodology): “More lattice plots may be found in (Bali, 2001; Bali et al., 1997).”
- Real-time Dynamics in U(1) Lattice Gauge Theories with Tensor Networks (2015, background): “In gauge theories hosting dynamical charges, there exists a critical length scale at which the confining string breaks, creating particle-antiparticle pairs which reduce the energy density in the string and give rise to the hadrons at the string edges [5].”
- The QCD running coupling (2016, background): “Lattice calculations for αV defined by the static Q–Q potential leads to an IR-freezing coupling [214].”
- The XYZ states: Experimental and theoretical status and perspectives (2019, unknown): “[351].”
- Quarkonia and their transitions (2007, background): “The well-measured static energy between a heavy quark-antiquark pair justifies the form of the nonrelativistic potential (Bali, 2001).”
- Glueballs, Hybrids, Multiquarks. Experimental facts versus QCD inspired concepts (2007, background): “The solid line represents a potential in the form V (r) = (4)3 3s r + b · r; from [140].”