Lattice perturbation theory in noncommutative geometry and parity anomaly in 3d noncommutative QED
Author(s) -
Jun Nishimura,
Miguel Angel Vázquez-Mozo
Publication year - 2003
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 - 10.1088/1126-6708/2003/01/075
Subject(s) - noncommutative geometry , noncommutative quantum field theory , physics , gauge theory , noncommutative algebraic geometry , fermion , parity (physics) , mathematical physics , dirac fermion , quantum mechanics
We formulate lattice perturbation theory for gauge theories in noncommutativegeometry. We apply it to three-dimensional noncommutative QED and calculate theeffective action induced by Dirac fermions. In particular "parity invariance"of a massless theory receives an anomaly expressed by the noncommutativeChern-Simons action. The coefficient of the anomaly is labelled by an integerdepending on the lattice action, which is a noncommutative counterpart of thephenomenon known in the commutative theory. The parity anomaly can also beobtained using Ginsparg-Wilson fermions, where the masslessness is guaranteedat finite lattice spacing. This suggests a natural definition of thelattice-regularized Chern-Simons theory on a noncommutative torus, which couldenable nonperturbative studies of quantum Hall systems.Comment: 31 pages. LaTeX, feynmf. Minor changes, references added and typos corrected. Final version published in JHE
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