1997
DOI: 10.1103/physrevd.55.3974
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Heavy quarkonia: Wilson area law, stochastic vacuum model, and dual QCD

Abstract: The QQ semirelativistic interaction in QCD can be simply expressed in terms of the Wilson loop and its functional derivatives. In this approach we present the QQ potential up to order 1/m 2 using the expressions for the Wilson loop given by the Wilson Minimal Area Law (MAL), the Stochastic Vacuum Model (SVM) and Dual QCD (DQCD). We confirm the original results given in the different frameworks and obtain new contributions. In particular we calculate up to order 1/m 2 the complete velocity dependent potential i… Show more

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Cited by 58 publications
(81 citation statements)
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“…Most of the 19.9 MeV deviation in the charmonium case arises from a 25 MeV discrepancy in the center-ofgravity of the 1P state. Much of this difference could probably be removed by a proper account of the spin-independent relativistic corrections [32].…”
Section: Richardson's Potential and The Spin-dependent Potentialsmentioning
confidence: 99%
“…Most of the 19.9 MeV deviation in the charmonium case arises from a 25 MeV discrepancy in the center-ofgravity of the 1P state. Much of this difference could probably be removed by a proper account of the spin-independent relativistic corrections [32].…”
Section: Richardson's Potential and The Spin-dependent Potentialsmentioning
confidence: 99%
“…The correct description of the fine structure of the heavy quarkonium mass spectrum requires the vanishing of the vector confinement contribution. This can be achieved by setting 1 + κ = 0, i.e., the total long-range quark chromomagnetic moment equals zero, which is in accord with the flux tube [19] and minimal area [16,20] models. One can see from Eq.…”
Section: Heavy Quarkonium and B C Meson Mass Spectramentioning
confidence: 99%
“…The model parameters can be also connected with the usual Coulomb plus linear potential [20,21,22] V (r) = − 4 α 3 r + b r + c…”
Section: Resultsmentioning
confidence: 99%
“…All parameters are correlated and compared with the nonrelativistic choices [20,21,22] The quark masses,were treated as fitting parameters in a limited sense. Suitable values, allowed within the experimental uncertainty in current quark masses [1], were selected.…”
Section: Introductionmentioning
confidence: 99%