Before sailing on a domain-wall sea
arXiv:hep-lat/0411007 · doi:10.1103/PhysRevD.71.034502
Abstract
We discuss the very different roles of the valence-quark and the sea-quark residual masses ( and ) in dynamical domain-wall fermions simulations. Focusing on matrix elements of the effective weak hamiltonian containing a power divergence, we find that can be a source of a much bigger systematic error. To keep all systematic errors due to residual masses at the 1% level, we estimate that one needs and , at a lattice spacing fm. The practical implications are that (1) optimal use of computer resources calls for a mixed scheme with different domain-wall fermion actions for the valence and sea quarks; (2) better domain-wall fermion actions are needed for both the sea and the valence sectors.
latex, 25 pages. Improved discussion in appendix, including correction of some technical mistakes; ref. added
References in corpus (1)
Cited by in corpus (11)
- Full nonperturbative QCD simulations with 2+1 flavors of improved staggered quarks
- 2+1 flavor domain wall QCD on a (2 fm)^3 lattice: light meson spectroscopy with Ls = 16
- Precise Determination of the I=2 pipi Scattering Length from Mixed-Action Lattice QCD
- Non-perturbative renormalization of quark bilinear operators and B_K using domain wall fermions
- Physics issues in simulations with dynamical overlap fermions
- Localization properties of lattice fermions with plaquette and improved gauge actions
- The Kaon B-parameter from Quenched Domain-Wall QCD
- The role of the double pole in lattice QCD with mixed actions
- Discretization effects and the scalar meson correlator in mixed-action lattice simulations
- The Kaon B-parameter in Mixed Action Chiral Perturbation Theory
- K to pi and K to 0 in 2+1 Flavor Partially Quenched Chiral Perturbation Theory