1989
DOI: 10.1016/0370-2693(89)91725-5
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Yukawa lattice theory and non-perturbative upper bounds to the fermion mass

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Cited by 81 publications
(64 citation statements)
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“…Since we have learned that decoupling of these modes by keeping their mass at the cutoff does not prevent the bound states from being formed and destroying the chiral structure of the theory, perhaps enforcing gauge fixing on the lattice would do the trick. This is precisely the proposal of the Rome group [31], although historically this proposal was quite independent from the reasoning I have presented here. Originally the motivation of the Rome group was to define a theory motivated by perturbative gauge fixing as a prescription for obtaining a full nonperturbative asymptotically free chiral gauge theory.…”
Section: The Rome Proposalsupporting
confidence: 63%
“…Since we have learned that decoupling of these modes by keeping their mass at the cutoff does not prevent the bound states from being formed and destroying the chiral structure of the theory, perhaps enforcing gauge fixing on the lattice would do the trick. This is precisely the proposal of the Rome group [31], although historically this proposal was quite independent from the reasoning I have presented here. Originally the motivation of the Rome group was to define a theory motivated by perturbative gauge fixing as a prescription for obtaining a full nonperturbative asymptotically free chiral gauge theory.…”
Section: The Rome Proposalsupporting
confidence: 63%
“…The model then becomes very similar to the Rome proposal [5], which uses Wilson fermions. A non-per-turbative test of this gauge fixing approach is difficult because of technical obstacles.…”
Section: Final Remarksmentioning
confidence: 77%
“…Many proposals are formulated such that local gauge invariance on the lattice is preserved [3,4,[7][8][9]11].For example, using a Wilson term to decouple the doublers, one introduces extra scalar fields to make this mass term gauge invariant. Alternatively one can sacrifice gauge invariance of the lattice model and transcribe the gauge fixed continuum action to the lattice [5,6]. This avoids introducing extra scalar fields, but requires Fadeev-Popov and gauge fixing terms.…”
Section: Introductionmentioning
confidence: 99%
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“…The question is how to restore it in the quantum theory . One can mimic the continuum methods closely, by attempting non-perturbative gauge fixing and adding counterterms to restore gauge invariance [6]. An alternative approach focuses on a possible dynamical restoration of gauge invariance [3,5].…”
Section: Introductionmentioning
confidence: 99%