Effective quark-antiquark potential for the constituent quark model

Journal Article · Tue Feb 14 23:00:00 EST 1995 · Physical Review, D (Particles Fields); (United States)

DOI:https://doi.org/10.1103/PhysRevD.51.1968· OSTI ID:6853253

Baker, M ^[1]; Ball, J S ^[2]; Zachariasen, F ^[3]

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1. University of Washington, Seattle, Washington 98105 (United States)
2. University of Utah, Salt Lake City, Utah 84112 (United States)
3. California Institute of Technology, Pasadena, California 91125 (United States)

We use Dual QCD to derive an effective potential to order (quark mass)[sup [minus]2] for a constituent quark and antiquark. This is done by expanding the dual QCD Lagrangian to second order in the [ital q[bar q]] spins and velocities around the static central potential, in which the quarks are both spinless and stationary. The field equations are then used to eliminate the dual gluon fields and the Higgs fields of dual QCD in favor of quark variables for an arbitrary but slowly moving [ital q[bar q]] pair with a Dirac string of arbitrary shape connecting them. The result is a Lagrangian, and therefore, a potential, which depends only on the [ital q[bar q]] positions, velocities, and spins. Dual QCD contains only three parameters, which can be determined from the vacuum energy density, the string tension, and the strength of the Coulomb singularity of the central potential. The only free parameters in the spin- and velocity-dependent part of the effective potential are, therefore, the masses of the [ital c] and [ital b] quarks. When inserted into a Schroedinger equation these potentials provide a complete effective constituent quark theory which can be used to calculate [ital q[bar q]] energy levels in terms of the masses and the masses can thereby be fixed (agreement with experiment is excellent). The various potential, spin-spin, spin-orbit, and spinless velocity dependent, can also in principle be compared to lattice calculations of the same quantities. For the spin-orbit case, for example, the agreement is good, although lattice results are not yet precise enough for a real comparison to be made. For the potentials proportional to the velocity squared lattice results do not yet exist. We also attempt to extend the use of these potentials to heavy-light quark-antiquark systems through use of the Salpeter equation and the Dirac equation. The results of this effort are described in two Appendices.

• DOE Contract Number: FG03-92ER40701
• OSTI ID: 6853253
• Journal Information: Physical Review, D (Particles Fields); (United States), Journal Name: Physical Review, D (Particles Fields); (United States) Vol. 51:4; ISSN PRVDAQ; ISSN 0556-2821
• Country of Publication: United States
• Language: English

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662240* -- Models for Strong Interactions-- (1992-)
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
ANGULAR MOMENTUM
ANTIMATTER
ANTIPARTICLES
BETHE-SALPETER EQUATION
BOSONS
COMPOSITE MODELS
DIFFERENTIAL EQUATIONS
DIRAC EQUATION
ELEMENTARY PARTICLES
ENERGY DENSITY
EQUATIONS
FERMIONS
FIELD EQUATIONS
FIELD THEORIES
FUNCTIONS
GLUONS
HIGGS BOSONS
LAGRANGIAN FUNCTION
MATHEMATICAL MODELS
MATTER
PARTIAL DIFFERENTIAL EQUATIONS
PARTICLE MODELS
PARTICLE PROPERTIES
POSTULATED PARTICLES
POTENTIALS
QUANTUM CHROMODYNAMICS
QUANTUM FIELD THEORY
QUARK MODEL
QUARKS
SCHROEDINGER EQUATION
SINGULARITY
SPIN
VELOCITY
WAVE EQUATIONS