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Can QCD Be a Perturbation Theory of Hadrons?
Author(s) -
Pervushin V. N.,
Kalinovsky Yu. L.,
Kallies W.,
Sarikova N. A.
Publication year - 1990
Publication title -
fortschritte der physik/progress of physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.469
H-Index - 71
eISSN - 1521-3978
pISSN - 0015-8208
DOI - 10.1002/prop.2190380502
Subject(s) - physics , glueball , quantum chromodynamics , ansatz , coupling constant , hamiltonian (control theory) , parton , bound state , hadron , quantum electrodynamics , particle physics , mathematical physics , quarkonium , mathematical optimization , mathematics
We have found that the S ‐matrix for atoms and hadrons depends on a gauge as the elementary particles are off mass‐shell in the bound states. The S ‐matrix for bound states one should to construct by the projection of the Belinfante energy‐momentum tensor on the Gauss equation solution for the time component with the time‐axis chosen as the eigenvector of the bound state total momentum operator. We have shown that this QCD Hamiltonian determined in infrared region by the rising potential ansatz, besides the parton model in the specific gauge, contains also the nonrelativistic potential model for heavy quarkonia, the chiral Lagrangians for light quarkonia with their spectrum, the glueball physics, and the small effective coupling constant in the whole region of transversal momenta.