1983
DOI: 10.1007/bf01027542
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The inverse problem of quantum mechanics for a linear potential

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Cited by 4 publications
(2 citation statements)
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“…It also took into account two important features that one expects from QCD, Heavy Flavor Symmetry (HFS) and Heavy Quark Spin Symmetry (HQSS), considering terms that are flavor and spin independent. The naive quark model from Cornell was fitted to the only 11 states that were known in 1978 and gave a quite good description of the charmonium and bottomonium spectrum at that time [25]. Not only that, the predictions were in quite good agreement with the experiments up to 2003, giving a prediction for 15 new states in the correct energy range.…”
Section: Introductionmentioning
confidence: 85%
See 1 more Smart Citation
“…It also took into account two important features that one expects from QCD, Heavy Flavor Symmetry (HFS) and Heavy Quark Spin Symmetry (HQSS), considering terms that are flavor and spin independent. The naive quark model from Cornell was fitted to the only 11 states that were known in 1978 and gave a quite good description of the charmonium and bottomonium spectrum at that time [25]. Not only that, the predictions were in quite good agreement with the experiments up to 2003, giving a prediction for 15 new states in the correct energy range.…”
Section: Introductionmentioning
confidence: 85%
“…[59]. The relation is given as γ = g s /2m (25) m being the mass of the pair created, which is usually a light pair. We consider a process where an initial hadron A decays into two final hadrons B and C. When we work in the center of mass system of the initial hadron, we have P A = P cm = 0, with P A the momentum of the initial hadron and P cm the total momentum of the final hadrons.…”
Section: The 3 P 0 Modelmentioning
confidence: 99%