1997
DOI: 10.1016/s0550-3213(97)80017-x
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Parity-invariant lattice regularization of a three-dimensional gauge-fermion system

Abstract: In three dimensions, the effective action for the gauge field induced by integrating out a massless Dirac fermion is known to give either a parity-invariant or a parity-violating result, depending on the regularization scheme. We construct a lattice formulation of the massless Dirac fermion using the overlap formalism. We show that the result is parity invariant in contrast to the formulation using Wilson fermions in the massless limit. This facilitates a non-perturbative study of three-dimensional massless Di… Show more

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Cited by 27 publications
(28 citation statements)
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“…See also[51] for an earlier work on the overlap formalism in odd dimensions, where a parity invariant phase choice has been made 5. This gauge violation was also concluded in ref [53],.…”
supporting
confidence: 59%
“…See also[51] for an earlier work on the overlap formalism in odd dimensions, where a parity invariant phase choice has been made 5. This gauge violation was also concluded in ref [53],.…”
supporting
confidence: 59%
“…When applied to Dirac fermions in even dimensions, an exact chiral symmetry is preserved and one can even derive a Dirac operator [11], which gives an explicit solution [12] to the Ginsparg-Wilson relation [13]. When applied to Dirac fermions in odd dimensions, parity invariance can be manifestly preserved [14], and a global gauge anomaly can be correctly reproduced [15]. These symmetries enable a lattice construction of supersymmetric gauge theories without fine-tuning [1,16].…”
Section: Introductionmentioning
confidence: 98%
“…This is quite reminiscent of the situation in commutative space-time with odd dimensions. There the parity anomaly conflicts with the gauge symmetry in some cases [25]. If one imposes the gauge invariance, one obtains the parity anomaly.…”
Section: Summary and Discussionmentioning
confidence: 99%
“…Comparing these results with our lattice construction, we observe a certain regularization dependence, which is reminiscent of the parity anomaly in commutative space-time with an odd number of dimensions (See Refs. [25] and references therein). We speculate that the gauge anomaly obtained in the continuum calculations might be cancelled by an appropriate counterterm in these cases.…”
Section: Introductionmentioning
confidence: 99%