Mixing of meson, hybrid, and glueball states

Preprint

2 October 2001

preprint
Published by arXiv in arXiv

https://doi.org/10.48550/arXiv.hep-ph/0110033

Abstract

The effective QCD Hamiltonian is constructed with the help of the background perturbation theory, and relativistic Feynman--Schwinger path integrals for Green's functions. The resulting spectrum displays mass gaps of the order of one GeV, when additional valence gluon is added to the bound state. Mixing between meson, hybrid, and glueball states is defined in two ways: through generalized Green's functions and via modified Feynman diagram technic giving similar answers. Results for mixing matrix elements are numerically not large (around 0.1 GeV) and agree with earlier analytic estimates and lattice simulations.

Keywords

MIXING BETWEEN MESON
PERTURBATION THEORY
QCD HAMILTONIAN
GLUEBALL STATES
EFFECTIVE QCD
FEYNMAN
GEV

All Related Versions

Version 1, 2001-10-02, ArXiv
Published version: Physics of Atomic Nuclei, 64 (10), 1876.

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