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Related papers: General chiral gauge theories

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We still extend the large class of Dirac operators decribing massless fermions on the lattice found recently, only requiring that such operators decompose into Weyl operators. After deriving general relations and constructions of operators,…

High Energy Physics - Lattice · Physics 2014-11-17 Werner Kerler

We only require generalized chiral symmetry and $\gamma_5$-hermiticity, which leads to a large class of Dirac operators describing massless fermions on the lattice, and use this framework to give an overview of developments in this field.…

High Energy Physics - Lattice · Physics 2009-11-07 Werner Kerler

Instead of the Ginsparg-Wilson (GW) relation we only require generalized chiral symmetry and show that this results in a larger class of Dirac operators describing massless fermions, which in addition to GW fermions and to the ones proposed…

High Energy Physics - Lattice · Physics 2009-11-07 Werner Kerler

We present a general formulation of chiral gauge theories, which admits Dirac operators with more general spectra, reveals considerably more possibilities for the structure of the chiral projections, and nevertheless allows appropriate…

High Energy Physics - Lattice · Physics 2007-05-23 Werner Kerler

Instead of the Ginsparg-Wilson relation only generalized chiral symmetry is required. The resulting much larger class of Dirac operators for massless fermions is investigated and a general construction for them is given. It is also shown…

High Energy Physics - Lattice · Physics 2009-11-07 Werner Kerler

We present a formulation of chiral gauge theories, which admits more general spectra of Dirac operators and reveals considerably more possibilities for the structure of the chiral projections. Our two forms of correlation functions both…

High Energy Physics - Lattice · Physics 2009-11-10 Werner Kerler

We combine a pair of independent Weyl fermions to compose a Dirac fermion on the four-dimensional Euclidean lattice. The obtained Dirac operator is antihermitian and does not reproduce anomaly under the usual chiral transformation. To…

High Energy Physics - Lattice · Physics 2007-05-23 Takanori Sugihara

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…

High Energy Physics - Lattice · Physics 2008-11-26 Peter Hasenfratz , Reto von Allmen

The Weyl fermion belonging to the real representation of the gauge group provides a simple illustrative example for L\"uscher's gauge-invariant lattice formulation of chiral gauge theories. We can explicitly construct the fermion…

High Energy Physics - Lattice · Physics 2009-10-31 Hiroshi Suzuki

We propose a nonperturbative formulation of chiral gauge theories. The method involves a `pre-regulation' of the gauge fields, which may be implemented on a lattice, followed by a computation of the chiral fermion determinant in the form of…

High Energy Physics - Theory · Physics 2008-02-03 Stephen D. H. Hsu

Starting from the Ginsparg-Wilson relation, a general construction of chiral gauge theories on the lattice is described. Local and global anomalies are easily discussed in this framework and a closed expression for the effective action can…

High Energy Physics - Lattice · Physics 2008-11-26 Martin Lüscher

Contents: 1. Introduction, 2. Chiral gauge theories & the gauge anomaly, 3. The regularization problem, 4. Weyl fermions from 4+1 dimensions, 5. The Ginsparg-Wilson relation, 6. Gauge-invariant lattice regularization of anomaly-free…

High Energy Physics - Theory · Physics 2017-08-23 Martin Lüscher

A family of theories which interpolate between vector and chiral Schwinger models is studied on the two--sphere $S^{2}$. The conflict between the loss of gauge invariance and global geometrical properties is solved by introducing a fixed…

High Energy Physics - Theory · Physics 2009-10-28 A. Bassetto , L. Griguolo

In a recent article Hasenfratz and von Allmen have suggested a fixed point action for two flavors of Weyl fermions on the lattice with gauge group SU(2). The block-spin transformation they use maps the chiral and vector symmetries of the…

High Energy Physics - Lattice · Physics 2008-11-26 Christof Gattringer , Markus Pak

Several simple asymptotically-free chiral gauge theories are studied. The only ``free parameters'' of our models are the choice of the gauge group and the matter Weyl fermion representations, and the relative magnitudes of the…

High Energy Physics - Theory · Physics 2026-05-12 Stefano Bolognesi , Kenichi Konishi , Matteo Orso

We show that gauge-transformation properties of correlation functions in chiral gauge theories on the finite lattice are determined in a general way.

High Energy Physics - Lattice · Physics 2007-05-23 Werner Kerler

We define Weyl fermions on a finite lattice in such a way that in the path integral the action is gauge invariant but the functional measure is not. Two variants of such a formulation are tested in perturbative calculation of the fermion…

High Energy Physics - Lattice · Physics 2014-11-17 Sergei V. Zenkin

A lattice derivative is defined as a discrete Fourier transform of momentum on a finite lattice. Species doublers are removed with anti-periodic boundary conditions. U(1) chiral transformation is modified to reproduce chiral anomaly. Chiral…

High Energy Physics - Lattice · Physics 2007-05-23 Takanori Sugihara

A manifestly gauge invariant formulation of chiral theories with fermions on the lattice is developed. It combines SLAC lattice derivative \cite{DWY}, \cite{ACS}, \cite{S} and generalized Pauli-Villars regularization \cite{FS}. The theory…

High Energy Physics - Theory · Physics 2009-10-28 A. A. Slavnov

We reconsider gauge-transformation properties in chiral gauge theories on the lattice observing all pertinent information and show that these properties are actually determined in a general way for any gauge group and for any value of the…

High Energy Physics - Lattice · Physics 2007-05-23 Werner Kerler
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