6533b854fe1ef96bd12aead2

RESEARCH PRODUCT

NNLO Unquenched Calculation of the b Quark Mass

V. GimenezGuido MartinelliLeonardo GiustiFederico Rapuano

subject

QuarkNuclear and High Energy PhysicsParticle physicsB physics gauge theory latticeComputationB physics QCD latticeHigh Energy Physics::LatticeBinding energyLattice field theoryFOS: Physical sciencesElementary particleBottom quarkPartícules (Física nuclear)RenormalonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)BibliographyPhysicsQuantum chromodynamicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)PropagatorFermionAtomic and Molecular Physics and OpticsFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyStrange matterHigh Energy Physics::Experiment

description

By combining the first unquenched lattice computation of the B-meson binding energy and the two-loop contribution to the lattice HQET residual mass, we determine the (\bar{{MS}}) (b)-quark mass, (\bar{m}_{b}(\bar{m}_{b})). The inclusion of the two-loop corrections is essential to extract (\bar{m}_{b}(\bar{m}_{b})) with a precision of ({\cal O}(\Lambda^{2}_{QCD}/m_{b})), which is the uncertainty due to the renormalon singularities in the perturbative series of the residual mass. Our best estimate is (\bar{m}_{b}(\bar{m}_{b}) = (4.26 \pm 0.09) {\rm GeV}), where we have combined the different errors in quadrature. A detailed discussion of the systematic errors contributing to the final number is presented. Our results have been obtained on a sample of (60) lattices of size (24^{3}\times 40) at (\beta =5.6), using the Wilson action for light quarks and the lattice HQET for the (b) quark, at two values of the sea quark masses. The quark propagators have been computed using the unquenched links generated by the T(\chi)L Collaboration.

https://dx.doi.org/10.48550/arxiv.hep-lat/0002007