Abstract:Here is presented a four-body potential model for q 2 q2 systems which includes both the spin and flavour degrees of freedom, extending the formalism presented already in the spin independent situation. This allows an application to a realistic situation, which is chosen to be K K scattering. It is seen that because of the gluonic effects in this multi-quark system, the K K attraction resulting from the quark-exchange mechanism gets appreciably decreased compared to that emerging through the naive two-body pot… Show more
“…After getting ω the constants and mesons sizes are obtained by using C = −(3/16)(2µω 2 ) and d = 1/2µω [20,27]. Hence the fitted parameters are m u = 0.1065, m c = 1.2877, C 1 = −0.0273, C 2 = −0.00615, C 3 = −0.002995 andC = 0.…”
Section: Finding the Cross-sectionsmentioning
confidence: 99%
“…[20,26], we multiply it by the matrix elements of the actual SU(3) color matrices. In these and related calculations [27,28] for meson-meson cross-sections and bindings, resonating group method (mentioned below in section II) has been employed to use the wave function of a single cluster of a quark antiquark pair. These wave functions are taken to be those of the quadratic confinement; each potential energy is also quadratic in the four papers.…”
We calculate the cross-sections for the processes ρJ/ψ → D 0D0 , ρJ/ψ → D 0D0 * (D 0 * D0 ) and ρJ/ψ → D 0 * D0 * using a QCD-motivated many-body overlap factor to modify the usual sum of two-body interaction model. The realistic Cornell potential has been used for pairwise interaction in the four quark Hamiltonian and noted to give lesser cross-sections as compared to the quadratic potential. The Resonating group method is employed along with the Born approximation which decouples its integral equations. It is pointed out that the additional QCD effect (a gluonic field ovelap factor) result in a significant suppression in the cross sections as compared to the more popular sum of two-body interaction.PACS numbers:
“…After getting ω the constants and mesons sizes are obtained by using C = −(3/16)(2µω 2 ) and d = 1/2µω [20,27]. Hence the fitted parameters are m u = 0.1065, m c = 1.2877, C 1 = −0.0273, C 2 = −0.00615, C 3 = −0.002995 andC = 0.…”
Section: Finding the Cross-sectionsmentioning
confidence: 99%
“…[20,26], we multiply it by the matrix elements of the actual SU(3) color matrices. In these and related calculations [27,28] for meson-meson cross-sections and bindings, resonating group method (mentioned below in section II) has been employed to use the wave function of a single cluster of a quark antiquark pair. These wave functions are taken to be those of the quadratic confinement; each potential energy is also quadratic in the four papers.…”
We calculate the cross-sections for the processes ρJ/ψ → D 0D0 , ρJ/ψ → D 0D0 * (D 0 * D0 ) and ρJ/ψ → D 0 * D0 * using a QCD-motivated many-body overlap factor to modify the usual sum of two-body interaction model. The realistic Cornell potential has been used for pairwise interaction in the four quark Hamiltonian and noted to give lesser cross-sections as compared to the quadratic potential. The Resonating group method is employed along with the Born approximation which decouples its integral equations. It is pointed out that the additional QCD effect (a gluonic field ovelap factor) result in a significant suppression in the cross sections as compared to the more popular sum of two-body interaction.PACS numbers:
“…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%
“…Using this approximation, we use the solutions (χ i (R i ), χ i (R i )) of eqs. (21)(22)(23)(24) in absence of interactions (meaning f = f a = f c = 0)…”
Section: Solving the Integral Equationsmentioning
confidence: 99%
“…At the quark level, this model II was noted to much reduce the chisquare of eq.(1). This model has been worked out in [22,23,24] till meson-level transition amplitudes. The dynamical calculations require a kinetic energy term as well.…”
We study meson-meson interactions using an extended q 2q2 (g) basis that allows calculating coupling of an ordinary meson-meson system to a hybrid-hybrid one. We use a potential model matrix in this extended basis which at quark level is known to provide a good fit to numerical simulations of a q 2q2 system in pure gluonic theory for static quarks in a selection of geometries. We use a combination of resonating group method formalism and Born approximation to include the quark motion using wave functions of a qq potential within a cluster. This potential is taken to be quadratic for ground states and has an additional smeared 1 r (Gaussian) for the matrix elements between hybrid mesons. For the parameters of this potential, we use values chosen to 1) minimize the error resulting from our use of a quadratic potential and 2) best fit the lattice data for differences of Σg and Πu configurations of the gluonic field between a quark and an antiquark. At the quark (static) level, including the gluonic excitations was noted to partially replace the need for introducing many-body terms in a multi-quark potential. We study how successful such a replacement is at the (dynamical) hadronic level of relevance to actual hard experiments. Thus we study effects of both gluonic excitations and many-body terms on mesonic transition amplitudes and the energy shifts resulting from the second order perturbation theory (i.e. from the respective hadron loops). The study suggests introducing both energy and orbital excitations in wave functions of scalar mesons that are modelled as meson-meson molecules or are supposed to have a meson-meson component in their wave functions.
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