Summary
«Chiral» symmetry for (2+1)-dimensional QCD is studied in large flavourN-limit, whereN is the number of two-component fermions. It is emphasized that, by finding a self-consistent approximate solution to Dyson-Schwinger equation withm≠0, «chiral» symmetry is spontaneously broken. Also the mass of the gauge bosons is generated by finding a non-zero value of the gauge self-energyII(k) atk=0.
Similar content being viewed by others
References
T. Appelquist, M. J. Bowick, D. Karabali andL. C. Rwijewardhana:Phys. Rev. D,33, 3704 (1986).
T. Appelquist, M. J. Bowick, D. Karabali andL. C. Rwijewardhana:Phys. Rev. D,33, 3774 (1986).
R. Pisarski:Phys. Rev. D,29, 2423 (1984).
T. Appelquist andR. Pisarski:Phys. Rev. D,23, 2305 (1981).
R. Jackiw andS. Templton:Phys. Rev. D,23, 2291 (1982).
J. Cornwall, R. Jackiw andT. Tomboulis:Phys. Rev. D,10, 2428 (1974).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Khalil, S.S. «Chiral» symmetry in (2+1)-dimensional QCD. Nuov Cim A 107, 689–696 (1994). https://doi.org/10.1007/BF02732078
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02732078