1991
DOI: 10.1016/0375-9474(91)90247-4
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A model for quark exchange in chromodynamics illustrated by a description of meson-meson scattering

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Cited by 19 publications
(47 citation statements)
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“…With the use of ground state potential v ij in the realistic coulombic plus linear form, it becomes impossible for us to solve the integral equations appearing below in eqs. (21)(22)(23)(24). Therefore we used the parametrization of the static pairwise two quark potential as v ij = Cr 2 ij + C, with i, j = 1, 2, 3, 4.…”
Section: Q 2 Q 2 Potential Model (In the Extended Basis)mentioning
confidence: 99%
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“…With the use of ground state potential v ij in the realistic coulombic plus linear form, it becomes impossible for us to solve the integral equations appearing below in eqs. (21)(22)(23)(24). Therefore we used the parametrization of the static pairwise two quark potential as v ij = Cr 2 ij + C, with i, j = 1, 2, 3, 4.…”
Section: Q 2 Q 2 Potential Model (In the Extended Basis)mentioning
confidence: 99%
“…In this simple harmonic potential, the parameters C is related to size (d) of wavefunction (ξ k ) through the relation C = − 3 16 1 d 4 = − 3 16 mω 2 with ω = 1 md 2 , and for consistency of the diagonal term of the integral eq. (21) C = 3 8 (4m + 3ω − 2M ) GeV [22] with M = 2m = 2.9588GeV being the mass of a charmonium meson. The parameter d is chosen in such a way to reduce the error resulting from a use of this quadratic potential instead of the realistic one.…”
Section: Q 2 Q 2 Potential Model (In the Extended Basis)mentioning
confidence: 99%
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