pith. machine review for the scientific record. sign in

arxiv: hep-lat/9801031 · v1 · submitted 1998-01-22 · ✦ hep-lat

Recognition: unknown

More about exactly massless quarks on the lattice

Authors on Pith no claims yet
classification ✦ hep-lat
keywords gammalatticemasslessquarkscertainconstructeddeterminantexactly
0
0 comments X
read the original abstract

In a previous publication [hep-lat/9707022] I showed that the fermion determinant for strictly massless quarks can be written on the lattice as $\det D$, where $D$ is a certain finite square matrix explicitly constructed from the lattice gauge fields. Here I show that $D$ obeys the Ginsparg-Wilson relation $D\gamma_5 D = D\gamma_5 +\gamma_5 D$.

This paper has not been read by Pith yet.

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Lattice fermion formulation via Physics-Informed Neural Networks: Ginsparg-Wilson relation and Overlap fermions

    hep-lat 2026-05 unverdicted novelty 7.0

    Physics-informed neural networks construct overlap fermions by optimizing to the Ginsparg-Wilson relation and autonomously discover both the standard and generalized Fujikawa-type versions of the relation.

  2. Lattice fermion formulation via Physics-Informed Neural Networks: Ginsparg-Wilson relation and Overlap fermions

    hep-lat 2026-05 unverdicted novelty 7.0

    Physics-Informed Neural Networks construct lattice Dirac operators satisfying the Ginsparg-Wilson relation, reproducing overlap fermions to high accuracy and discovering a Fujikawa-type generalized relation via algebr...

  3. Taste-splitting mass and edge modes in $3+1$ D staggered fermions

    hep-lat 2026-04 unverdicted novelty 7.0

    A kink in a one-link mass term for 3+1D staggered fermions creates a 2+1D domain wall with two-flavor massless Dirac fermions protected by SU(2) and parity, realizing the parity anomaly from the UV lattice Hamiltonian.