Abstract
We consider HQET including the first order correction in 1/m. A strategy for the computation of the b-quark mass following the scheme (Equation Presented) is discussed. Only two quantities Φ∗;1/2 have to be considered in order to match QCD and HQET, since the spin-dependent interaction is easily eliminated due to the spin symmetry of the static theory. Quite simple formulae relate the renormalization group invariant b-quark mass (M b) to the B-meson mass. All entries in these formulae are non-perturbatively defined and can be computed in the continuum limit of the lattice regularized theory. For the numerically most critical part, we illustrate the cancellation of power divergences by a numerical example. Numerical results for the 1/m correction to M b, are presented in a companion talk.
| Original language | English |
|---|---|
| Journal | P o S - Proceedings of Science |
| Volume | 20 |
| ISSN | 1824-8039 |
| DOIs | |
| Publication status | Published - 2005 |
| Externally published | Yes |
| Event | 23rd International Symposium on Lattice Field Theory, LAT 2005 - Dublin, Ireland Duration: 25. Jul 2005 → 30. Jul 2005 |
Conference
| Conference | 23rd International Symposium on Lattice Field Theory, LAT 2005 |
|---|---|
| Country/Territory | Ireland |
| City | Dublin |
| Period | 25/07/2005 → 30/07/2005 |
Funding
∗This work has been supported by the Deutsche Forschungsgemeinschaft (DFG) in SFB Transregio 9 “Computational Particle Physics”. †Speaker.
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