The Renormalizability of Gauge Theory on a Non-Commutative Plane
Author(s) -
Wolfgang Bietenholz,
Frank Hofheinz,
Jun Nishimura
Publication year - 2002
Publication title -
journal of high energy physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.998
H-Index - 261
eISSN - 1126-6708
pISSN - 1029-8479
DOI - 10.1088/1126-6708/2002/09/009
Subject(s) - physics , mathematical physics , gauge theory , lattice gauge theory , scaling limit , commutative property , wilson loop , renormalization , hamiltonian lattice gauge theory , scaling , lattice (music) , quantum mechanics , mathematics , geometry , pure mathematics , acoustics
We perform a non-perturbative study of pure gauge theory in a two dimensionalnon-commutative (NC) space. On the lattice, it is equivalent to the twistedEguchi-Kawai model, which we simulated at N ranging from 25 to 515. We observea clear large-N scaling for the 1- and 2-point function of Wilson loops, aswell as the 2-point function of Polyakov lines. The 2-point functions agreewith a universal wave function renormalization. Based on a Morita equivalence,the large-N double scaling limit corresponds to the continuum limit of NC gaugetheory, so the observed large-N scaling demonstrates the non-perturbativerenormalizability of this NC field theory. The area law for the Wilson loopsholds at small physical area as in commutative 2d planar gauge theory, but atlarge areas we find an oscillating behavior instead. In that regime the phaseof the Wilson loop grows linearly with the area. This agrees with theAharonov-Bohm effect in the presence of a constant magnetic field, identifiedwith the inverse non-commutativity parameter.Comment: 18 pages, 6 figures, final version published in JHE
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