Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCD
arXiv:hep-lat/0702017 · doi:10.1016/j.nuclphysb.2007.03.051
Abstract
We simulate two variants of quenched twisted mass QCD (tmQCD), with degenerate Wilson quarks of masses equal to or heavier than half the strange quark mass. We use Ward identities in order to measure the twist angles of the theory and thus check the quality of the tuning of mass parameters to a physics condition which stays constant as the lattice spacing is varied. Flavour symmetry breaking in tmQCD is studied in a framework of two fully twisted and two standard Wilson quark flavours, tuned to be degenerate in the continuum. Comparing pseudoscalar masses, obtained from connected quark diagrams made of tmQCD and/or standard Wilson quark propagators, we confirm that flavour symmetry breaking effects, which are at most 5%, decrease as we approach the continuum limit. We also compute the pseudoscalar decay constant in the continuum limit, with reduced systematics. As a consequence of improved tuning of the mass parameters at , we reanalyse our previous results. Our main phenomenological findings are and .
41 pages, figures included, one reference added. Final version as accepted for publication on Nucl.Phys.B
References in corpus (3)
- K^0-\bar K^0 mixing beyond the standard model and CP-violating electroweak penguins in quenched QCD with exact chiral symmetry
- Non-perturbative renormalization of static-light four-fermion operators in quenched lattice QCD
- Non-perturbative renormalisation of left-left four-fermion operators with Neuberger fermions
Cited by in corpus (10)
- FLAG Review 2021
- Twisted mass lattice QCD
- FLAG Review 2024
- BK-parameter from Nf = 2 twisted mass lattice QCD
- Non-perturbative renormalization of static-light four-fermion operators in quenched lattice QCD
- Non-perturbative renormalisation of Delta F=2 four-fermion operators in two-flavour QCD
- Non-leptonic kaon decays at large
- Progress in kaon physics on the lattice
- K^0-\bar{K}^0 Mixing Beyond the SM from Nf=2 tmQCD
- K* vector and tensor couplings from Nf = 2 tmQCD