activity
20022013
most citedTwisted mass QCD and lattice approaches to the rule

50 citations · 161 across the 10 of their papers we have counts for

collaborators

11 papers

hep-lat2013

Renormalization of HQET operators: O() improvement and matching with QCD

M. Papinutto, G. Herdoiza, C. Pena +1

We determine a basis of dimension-7 operators which arise at O() in the Symanzik expansion of the operators with static heavy quarks. We consider both Wilson-like and Gin…

hep-lat2008★ 9 cited

Testing chiral effective theory with quenched lattice QCD

L. Giusti, P. Hernandez, S. Necco +3

We investigate two-point correlation functions of left-handed currents computed in quenched lattice QCD with the Neuberger-Dirac operator. We consider two lattice spacings a~0.09,0…

hep-lat2007★ 1 cited

Non-perturbative renormalisation of four-fermion operators in N_f=2 QCD

P. Dimopoulos, G. Herdoiza, F. Palombi +4

We present results for the non-perturbative renormalisation of four-fermion operators with two flavours of dynamical quarks. We consider both fully relativistic left current-left c…

hep-lat2007★ 1 cited

First quenched results for the matrix elements of the B_{B_s} mixing parameter in the static limit from tmQCD

F. Palombi, M. Papinutto, C. Pena +1

We report on a non-perturbative study of the scale-dependent renormalization factors of a multiplicatively renormalizable basis of Delta B=2 parity-odd four-fermion operators in qu…

hep-lat2007★ 48 cited

Non-perturbative renormalization of static-light four-fermion operators in quenched lattice QCD

Filippo Palombi, Mauro Papinutto, Carlos Pena +1

We perform a non-perturbative study of the scale-dependent renormalization factors of a multiplicatively renormalizable basis of parity-odd four-fermion operators in quenc…

hep-lat2007★ 23 cited

Flavour symmetry restoration and kaon weak matrix elements in quenched twisted mass QCD

P. Dimopoulos, J. Heitger, F. Palombi +3

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…