Do multiquark hadrons exist
Journal Article
·
· Phys. Rev. Lett.; (United States)
The qqq-barq-bar system has been examined by solving the four-particle Schroedinger equation variationally. The main findings are that: (1) qqq-barq-bar bound states normally do not exist, (2) the cryptoexotic 0/sup + +/ sector of this system with KK-bar quantum numbers is probably the only exception to (1) and its bound states can be identified with the S* and delta just below KK-bar threshold, (3) qqq-barq-bar bound states provide a model for the weak binding and color-singlet clustering observed in nuclei, and (4) there is no indication that this system has strong resonances.
- Research Organization:
- Department of Physics, University of Toronto, Toronto, Ontario M5S 1A7, Canada
- OSTI ID:
- 5382816
- Journal Information:
- Phys. Rev. Lett.; (United States), Vol. 48:10
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
MESON RESONANCES
COLOR MODEL
QUARKS
FOUR-BODY PROBLEM
BOUND STATE
HAMILTONIANS
PARTICLE WIDTHS
QUANTUM NUMBERS
SCHROEDINGER EQUATION
VARIATIONAL METHODS
BOSONS
COMPOSITE MODELS
DIFFERENTIAL EQUATIONS
ELEMENTARY PARTICLES
EQUATIONS
HADRONS
MANY-BODY PROBLEM
MATHEMATICAL MODELS
MATHEMATICAL OPERATORS
MESONS
PARTIAL DIFFERENTIAL EQUATIONS
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QUARK MODEL
RESONANCE PARTICLES
WAVE EQUATIONS
645205* - High Energy Physics- Particle Interactions & Properties-Theoretical- Strong Interactions
Baryon No. = 0- (-1987)
MESON RESONANCES
COLOR MODEL
QUARKS
FOUR-BODY PROBLEM
BOUND STATE
HAMILTONIANS
PARTICLE WIDTHS
QUANTUM NUMBERS
SCHROEDINGER EQUATION
VARIATIONAL METHODS
BOSONS
COMPOSITE MODELS
DIFFERENTIAL EQUATIONS
ELEMENTARY PARTICLES
EQUATIONS
HADRONS
MANY-BODY PROBLEM
MATHEMATICAL MODELS
MATHEMATICAL OPERATORS
MESONS
PARTIAL DIFFERENTIAL EQUATIONS
PARTICLE MODELS
PARTICLE PROPERTIES
POSTULATED PARTICLES
QUANTUM OPERATORS
QUARK MODEL
RESONANCE PARTICLES
WAVE EQUATIONS
645205* - High Energy Physics- Particle Interactions & Properties-Theoretical- Strong Interactions
Baryon No. = 0- (-1987)