Abstract
A simultaneous Schroedinger fit of the spectra of both light and heavy mesons by an empirical power-law potential of the form V(r) = -8.0248+6.757r/sup 0.1/ (in GeV units) is obtained by extending a previous fit of the spectra of self-conjugate mesons to that of non-self-conjugate mesons containing up, down, and strange quarks. In spite of the smallness of the constituent quark masses involved, the nonrelativistic fit for the light mesons is astonishingly good.
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