Chiral fermions on the lattice
arXiv:hep-lat/9909042 · doi:10.1016/S0920-5632(00)91596-2
Abstract
Chiral fermions resisted being put on the lattice for twenty years. This raised the suspicion that asymptotically free chiral gauge theories were not renormalizable outside perturbation theory and therefore could not be mathematically extended to infinite energies. During the last several years the situation has reversed itself. Today we believe that all the essential ingredients for a full lattice definition of non-anomalous chiral gauge theories are in place within the overlap construction. This construction is based on earlier work by Callan and Harvey, by Kaplan and by Frolov and Slavnov. It can be reinterpreted as coming from the Ginsparg-Wilson relation, but, at the moment, it is a unique construction and therefore might also be the way by which Nature itself regularizes chiral fermions. This is yet another instance in which lattice field theory makes a potentially important contribution to fundamental particle physics.
10 pages, latex, espcrc2.sty
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- Progress using generalized lattice Dirac operators to parametrize the Fixed-Point QCD action
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- Nonperturbative renormalization of composite operators with overlap fermions
- Solving the local cohomology problem in U(1) chiral gauge theories within a finite lattice
- A simple construction of fermion measure term in U(1) chiral lattice gauge theories with exact gauge invariance
- Perturbative renormalization of the first two moments of non-singlet quark distributions with overlap fermions
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- A numerical solution to the local cohomology problem in U(1) chiral gauge theories
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