TY - JOUR
T1 - Non-linear σ models
T2 - A perturbative approach to symmetry restoration
AU - McKane, Alan
AU - Stone, Michael
N1 - Funding Information:
One of us (M.S.) would like to thank M.I.T. for hospitality during the first phase of this work and also St. Johns College, Cambridge for a research fellowship.
PY - 1980
Y1 - 1980
N2 - We examine the extent to which pertubation theory, about the naive Goldstone vacuum in two dimensions, is able to reveal the true state of affairs - that there are no Goldstone modes and that the symmetry is restored for arbitrarily small coupling constant. We exploit the recent observation, by Elitzur, of the infrared finiteness of globally invariant Green functions to compute them to third non-trivial order in a variety of models. Applying the renormalization group to improve these calculations we argue that one can see cluster decomposition beginning to restore the symmetry. The perturbation theory's ignorance of the global topology means that we cannot follow the decay of the Green function out to infinity because of a "non-perturbative barrier". We comment on the relevance of this to "perturbative confinement" in QCD. We also examine the way in which the global topology influences the phase diagrams when we add the two-dimensional analogue of Higgs fields.
AB - We examine the extent to which pertubation theory, about the naive Goldstone vacuum in two dimensions, is able to reveal the true state of affairs - that there are no Goldstone modes and that the symmetry is restored for arbitrarily small coupling constant. We exploit the recent observation, by Elitzur, of the infrared finiteness of globally invariant Green functions to compute them to third non-trivial order in a variety of models. Applying the renormalization group to improve these calculations we argue that one can see cluster decomposition beginning to restore the symmetry. The perturbation theory's ignorance of the global topology means that we cannot follow the decay of the Green function out to infinity because of a "non-perturbative barrier". We comment on the relevance of this to "perturbative confinement" in QCD. We also examine the way in which the global topology influences the phase diagrams when we add the two-dimensional analogue of Higgs fields.
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U2 - 10.1016/0550-3213(80)90396-X
DO - 10.1016/0550-3213(80)90396-X
M3 - Article
AN - SCOPUS:0642328083
SN - 0550-3213
VL - 163
SP - 169
EP - 188
JO - Nuclear Physics, Section B
JF - Nuclear Physics, Section B
IS - C
ER -