2008
DOI: 10.1088/1126-6708/2008/02/079
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Towards Weyl fermions on the lattice without artefacts

Abstract: In spite of the breakthrough in non-perturbative chiral gauge theories during the last decade, the present formulation has stubborn artefacts. Independently of the fermion representation one is confronted with unwanted CP violation and infinitely many undetermined weight factors. Renormalization group identifies the culprit. We demonstrate the procedure on Weyl fermions in a real representation.

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Cited by 17 publications
(28 citation statements)
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“…Note that the above remarks refer to the continuum CP transformation: recently ref. 61 argued that in the trivial topological sector it is possible to define a lattice-modified version of CP, (which, like the modified chiral symmetry, reduces to the usual continuum CP-transform), under which the chiral action (26) (and measure) is invariant; see also 62,63 .…”
Section: Problems With Ginsparg-wilson Fermions In Chiral Gauge Theoriesmentioning
confidence: 99%
“…Note that the above remarks refer to the continuum CP transformation: recently ref. 61 argued that in the trivial topological sector it is possible to define a lattice-modified version of CP, (which, like the modified chiral symmetry, reduces to the usual continuum CP-transform), under which the chiral action (26) (and measure) is invariant; see also 62,63 .…”
Section: Problems With Ginsparg-wilson Fermions In Chiral Gauge Theoriesmentioning
confidence: 99%
“…While this could still be controlled using extrapolations, the second problem cannot be circumvented. The lattice regularization introduces a gauge anomaly in the weak interactions, as it is incompatible with parity violation [18]. This problem is unresolved despite many efforts [19][20][21][22][23].…”
Section: Introductionmentioning
confidence: 99%
“…. 9 The precise definition of "all possible continuous paths" is unimportant as long as, for each path contained within the sum, the path ordered integration over the gauge fields defined in equation (30) remains differentiable, starts and terminates at the required locations, and contains the shortest path between the two points. It could, for example, either be defined to be the paths bound within the hypercube around x or not.…”
Section: The Blockingmentioning
confidence: 99%
“…A possible solution to this problem, which uses a lattice redefinition of the Parity operator, a different approach to that presented here, was recently suggested in[29]; see also the attempts using the perfect action formalism in[30,31]. An older overview of chiral gauge theories on the lattice can be found in[32].…”
mentioning
confidence: 99%