“…By (2.1) and (2.7) we then find for a low particle velocity 10) For g = 2, the above equation becomes 11) which is of the same magnitude but opposite sign from the pure Thomas term. Discussing QCD in an electrodynamic context is not unreasonable in this model of quark dynamics given the assumptions we make about the physical fields.…”
Section: Buchmüller's Picture Of the Spin-orbit Interaction In Qcdmentioning
confidence: 87%
“…If the confinement is pure time component vector we substitute (4.14) into (4.6) to obtain (4.15) In the case of scalar confinement we take (4.16) A similar reduction gives (4.17) Finally, the low quark velocity expansion of the Wilson minimal area law provides the effective Hamiltonian implied by QCD [11], (4.18) We observe that our model, scalar confinement, and low quark velocity expansion of the Wilson loop model [11] all have the pure Thomas spin-orbit interaction. The Darwin terms differ but are sensitive to the ordering prescription applied to symmetrize the operators.…”
Starting from Buchmüller's observation that a chromoelectric flux tube meson will exhibit only the Thomas type spin-orbit interaction, we show that a model built upon the related assumption that a quark feels only a constant radial chromoelectric field in its rest frame implies a complete relativistic effective Hamiltonian that can be written explicitly in terms of quark canonical variables. The model yields linear Regge trajectories and exhibits some similarities to scalar confinement, but with the advantage of being more closely linked to QCD.
“…By (2.1) and (2.7) we then find for a low particle velocity 10) For g = 2, the above equation becomes 11) which is of the same magnitude but opposite sign from the pure Thomas term. Discussing QCD in an electrodynamic context is not unreasonable in this model of quark dynamics given the assumptions we make about the physical fields.…”
Section: Buchmüller's Picture Of the Spin-orbit Interaction In Qcdmentioning
confidence: 87%
“…If the confinement is pure time component vector we substitute (4.14) into (4.6) to obtain (4.15) In the case of scalar confinement we take (4.16) A similar reduction gives (4.17) Finally, the low quark velocity expansion of the Wilson minimal area law provides the effective Hamiltonian implied by QCD [11], (4.18) We observe that our model, scalar confinement, and low quark velocity expansion of the Wilson loop model [11] all have the pure Thomas spin-orbit interaction. The Darwin terms differ but are sensitive to the ordering prescription applied to symmetrize the operators.…”
Starting from Buchmüller's observation that a chromoelectric flux tube meson will exhibit only the Thomas type spin-orbit interaction, we show that a model built upon the related assumption that a quark feels only a constant radial chromoelectric field in its rest frame implies a complete relativistic effective Hamiltonian that can be written explicitly in terms of quark canonical variables. The model yields linear Regge trajectories and exhibits some similarities to scalar confinement, but with the advantage of being more closely linked to QCD.
“…[14,15], since the spectral representation of V d (r) consists of the same amplitudes and the energy gaps. We plan to present this result as well as the other velocity-dependent potentials at O(1/m 2 ) in a separate publication.…”
Section: Discussionmentioning
confidence: 99%
“…Further, by integrating out the scale mv, where v is quark velocity, one arrives at a framework called potential NRQCD (pN-RQCD) [7,8,9,10], where the static potential emerges as the leading-order contribution, followed by relativistic corrections in powers of 1/m. The potential at O(1/m 2 ) contains the leading order spin-dependent corrections [11,12,13] and the velocity-dependent potentials [14,15]. Perturbation theory may be applied to the determination of these potentials to some extent.…”
The relativistic correction to the QCD static inter-quark potential at O(1/m) is investigated nonperturbatively for the first time by using lattice Monte Carlo QCD simulations. The correction is found to be comparable with the Coulombic term of the static potential when applied to charmonium, and amounts to one-fourth of the Coulombic term for bottomonium.
“…[8], if full relativistic kinematics is kept, but the spin dependent terms are neglected, it becomes identical to the potential of the relativistic flux tube model [3].…”
Abstract. In line with some previous works, we study in this paper the meson spectrum in the framework of a second order quark-antiquark Bethe-Salpeter formalism which includes confinement. An analytic one loop running coupling constant α s (Q), as proposed by Shirkov and Sovlovtsov, is used in the calculations. As for the quark masses, the case of a purely phenomenological running mass for the light quarks in terms of the c. m. momentum is further investigated. Alternatively a more fundamental expression m P (Q) is introduced for light and strange quarks, combining renormalization group and analyticity requirements with an approximate solution of the Dyson-Schwinger equation. The use of such running coupling constant and masses turns out to be essential for a correct reproduction of the the light pseudoscalar mesons.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.