How to calculate the quantum part of the truly nonperturbative Yang-Mills vacuum energy density in the axial gauge QCD

Citation
V. Gogohia et G. Kluge, How to calculate the quantum part of the truly nonperturbative Yang-Mills vacuum energy density in the axial gauge QCD, PHYS LETT B, 477(1-3), 2000, pp. 387-395
Citations number
42
Categorie Soggetti
Physics
Journal title
PHYSICS LETTERS B
ISSN journal
03702693 → ACNP
Volume
477
Issue
1-3
Year of publication
2000
Pages
387 - 395
Database
ISI
SICI code
0370-2693(20000323)477:1-3<387:HTCTQP>2.0.ZU;2-N
Abstract
Using the effective potential approach for composite operators, we have for mulated a general method how to calculate the truly nonperturbative vacuum energy density in the axial gauge QCD quantum models of its ground state. I t is defined as integrated out the truly nonperturbative part of the fall g luon propagator over the deep infrared region (soft momentum region). The n ontrivial minimization procedure makes it possible to determine the value o f the soft cutoff in terms of the corresponding nonperturbative scale param eter which is inevitably presented in any nonperturbative model for the ful l gluon propagator. If the chosen Ansatz for the full gluon propagator is a realistic one, then our method uniquely determines the truly vacuum energy density, which is always finite, automatically negative and it has no imag inary part (stable vacuum). We illustrate it by considering the Abelian Hig gs model of dual QCD ground state. We have explicitly shown that the vacuum of this model without string contributions is unstable against quantum cor rections. (C) 2000 Published by Elsevier Science B.V. All rights reserved.