Effective field theories for heavy quarkonium
By N. Brambilla, A. Pineda, J. Soto, A. Vairo. 2004
490 citations recorded by the source corpus.
We briefly review how nonrelativistic effective field theories give us a definition of the QCD potentials and a coherent field-theory-derived quantum-mechanical scheme to calculate the properties of bound states made by two or more heavy quarks. In this framework heavy quarkonium properties depend only on the QCD parameters (quark masses and αs) and nonpotential corrections are systematically accounted for. The relation between the form of the nonperturbative potentials and the low-energy QCD dynamics is also discussed.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/1c1de703a4fc117249f9abb4cba124297c4d1c33
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In Nuclear and High Energy Physics
Citations in the corpus
- Thermal bottomonium suppression at RHIC and LHC (2011, methodology): “At zero temperature, since the velocity of the quarks in the bound state is small (v c), quarkonium can be understood in terms of non-relativistic potential models such as the Cornell potential which can be derived directly from QCD using effective field theory [10–12].”
- Systematic Scale-Setting to All Orders: The Principle of Maximum Conformality and Commensurate Scale Relations (2013, background): “This IR divergence is a feature of pQCD and is canceled by non-perturbative contributions from the ’ultra-soft’ region [75, 76], which is controlled by the domain of color-confinement.”
- Baryons as relativistic three-quark bound states (2016, background): “[120, 121] for reviews, and on the other hand via lattice QCD, see e.”
- Heavy-quark QCD exotica (2016, background): “Quantum Chromodynamics (QCD) has long been the accepted quantum field theory of the strong nuclear force responsible for holding atomic nuclei together.”
- Heavy quarkonium in extreme conditions (2019, unknown): “[33].”
- The XYZ states: Experimental and theoretical status and perspectives (2019, background): “calls for the construction of a tower of non-relativistic EFTs [631], see Fig.”