For the abelian Yang-Mills theory, a one-to-one correspondence is established between continuum gauge potentials and compatible lattice configurations on an infinite sequence of finer and finer lattices. The compatibility is given by a block spin transformation determining the configuration on a lattice in terms of the configuration on any finer lattice. Thus the configuration on any single lattice is not an “approximation” to the continuum field, but rather a subset of the variables describing the field.It is proven that the Wilson actions on the lattices monotonically increase to the continuum action as one passes to finer and finer lattices. Configurations that minimize the continuum action, subject to having the variables fixed on some lattice, are studied.
[1]
Paul Federbush.
A phase cell approach to Yang-Mills theory
,
1987
.
[2]
J. Imbrie,et al.
Renormalization of the Higgs model: Minimizers, propagators and the stability of mean field theory
,
1985
.
[3]
Paul Federbush.
A Phase Cell Approach to Yang-Mills Theory I. Modes, Lattice-Continuum Duality*
,
1986
.
[4]
A phase cell approach to Yang-Mills theory
,
1987
.
[5]
T. Bałaban.
Propagators and renormalization transformations for lattice gauge theories. I
,
1984
.
[6]
K. Gawȩdzki,et al.
A rigorous block spin approach to massless lattice theories
,
1980
.
[7]
Averaging operations for lattice gauge theories
,
1985
.