We compute the static-light baryon spectrum with Nf = 2 flavors of sea quarks using Wilson twisted mass lattice QCD. As light valence quarks we consider quarks, which have the same mass as the sea quarks with corresponding pion masses in the range 340MeV<∼ mPS<∼ 525MeV, as well as partially quenched quarks, which have the mass of the physical s quark. We extract masses of states with isospin I = 0,1/2,1, with strangeness S = 0,−1,−2, with angular momentum of the light degrees of freedom j = 0,1 and with parity P = +,−. We present a preliminary extrapolation in the light u/d and an interpolation in the heavy b quark mass to the physical point and compare with available experimental results
Contribution at the XXVIII International Symposium on Lattice Field Theory, Lattice2010, June 14-19,...
By the ETM Collaboration, 24 pages, 24 figuresThe masses of the low lying baryons are evaluated usin...
We present first results on the octet and decuplet strange baryon spectrum with Nf = 2 + 1 + 1 twis...
We compute the static-light baryon spectrum with Nf = 2 flavors of sea quarks using Wilson twisted m...
We compute the static-light meson spectrum with N_f = 2 flavours of sea quarks using Wilson twisted ...
We compute the static-light meson spectrum using two-flavor Wilson twisted mass lattice QCD. We have...
We present results for the static-light meson from unquenched lattice QCD. The unquenched gauge conf...
We present results for the spectrum of static-light mesons from Nf=2 lattice QCD. These results were...
Submitted to Cornell University’s online archive www.arXiv.org in 2006 by Justin Foley.Post-print so...
The isospin, spin and parity dependent potential of a pair of static-light mesons is computed using ...
Version as appeared in Phys. Rev. D 90, 074501 (2014); 35 pages and 27 figuresThe masses of the low ...
peer-reviewedWe present preliminary results for the static-light meson and baryon spectra for Nf = 2...
Contribution at the XXVIII International Symposium on Lattice Field Theory, Lattice2010, June 14-19,...
The masses of the low-lying baryons are evaluated using a total of ten ensembles of dynamical twiste...
The masses of the low lying baryons are evaluated using a total of ten ensembles of dynamical twiste...
Contribution at the XXVIII International Symposium on Lattice Field Theory, Lattice2010, June 14-19,...
By the ETM Collaboration, 24 pages, 24 figuresThe masses of the low lying baryons are evaluated usin...
We present first results on the octet and decuplet strange baryon spectrum with Nf = 2 + 1 + 1 twis...
We compute the static-light baryon spectrum with Nf = 2 flavors of sea quarks using Wilson twisted m...
We compute the static-light meson spectrum with N_f = 2 flavours of sea quarks using Wilson twisted ...
We compute the static-light meson spectrum using two-flavor Wilson twisted mass lattice QCD. We have...
We present results for the static-light meson from unquenched lattice QCD. The unquenched gauge conf...
We present results for the spectrum of static-light mesons from Nf=2 lattice QCD. These results were...
Submitted to Cornell University’s online archive www.arXiv.org in 2006 by Justin Foley.Post-print so...
The isospin, spin and parity dependent potential of a pair of static-light mesons is computed using ...
Version as appeared in Phys. Rev. D 90, 074501 (2014); 35 pages and 27 figuresThe masses of the low ...
peer-reviewedWe present preliminary results for the static-light meson and baryon spectra for Nf = 2...
Contribution at the XXVIII International Symposium on Lattice Field Theory, Lattice2010, June 14-19,...
The masses of the low-lying baryons are evaluated using a total of ten ensembles of dynamical twiste...
The masses of the low lying baryons are evaluated using a total of ten ensembles of dynamical twiste...
Contribution at the XXVIII International Symposium on Lattice Field Theory, Lattice2010, June 14-19,...
By the ETM Collaboration, 24 pages, 24 figuresThe masses of the low lying baryons are evaluated usin...
We present first results on the octet and decuplet strange baryon spectrum with Nf = 2 + 1 + 1 twis...