B-meson physics with domain-wall light quarks and relativistic heavy quarks
نویسندگان
چکیده
We propose to compute B-meson weak matrix elements needed to constrain the CKM unitarity triangle and test the Standard Model in the quark flavor sector using the 2+1 flavor dynamical domain-wall fermion gauge field configurations generated by the LHP, RBC, and UKQCD Collaborations and relativistic b quarks. In the upcoming year we aim to finish our calculation of the B-meson leptonic decay constants fBd and fBs , the B − B0 mixing matrix elements, and their ratio, ξ ≡ fBs √ BBs/fBd √ BBd . The SU(3)-breaking ratio ξ provides an important constraint on the apex of the CKM triangle and was therefore highlighted as a key goal in flavor physics in the USQCD Collaboration’s 2007 white paper. We will also calculate the B → π`ν form factor using the same method, which will enable a determination of the CKM Matrix element |Vub|. Calculations of |Vub| are particularly critical due to the worrisome ≈ 3σ tension between inclusive and exclusive determinations. For all of these B-meson weak matrix elements we expect to obtain precise results that are competitive with other approaches, and that will place strong constraints on the CKM unitarity triangle fits. Our calculations will provide independent and valuable crosschecks of the results by HPQCD and Fermilab/MILC who both use the same set of gauge field configurations (different than those used in this proposal). We request the equivalent of 3.3 million jpsi core-hours on the Fermilab clusters plus 100 Tbytes of tape storage (the equivalent of ∼ 0.3 million jpsi core-hours) and 0.4 Tbytes of disk storage (the equivalent of ∼ 12k jpsi core-hours) for this project.
منابع مشابه
Relativistic NJL Model with Light and Heavy Quarks
We study the Nambu-Jona-Lasinio model with light and heavy quarks in a relativistic approach. We emphasize relevant regularization issues as well as the transition from light to heavy quarks. The approach of the electromagnetic meson form factor to the Isgur-Wise function in the heavy quark limit is
متن کاملB-meson decay constants and B −B0-mixing with domain-wall light and relativistic heavy quarks
We propose to continue and finish our determination of the B-meson leptonic decay constants fBd and fBs , the B−B0 mixing matrix elements, and their ratio, ξ ≡ fBs √ BBs/fBd √ BBd , on the 2+1 flavor dynamical domain-wall fermion gauge field configurations generated by the LHP, RBC, and UKQCD Collaborations. Using the relativistic heavy quark action we expect to obtain precise results which wil...
متن کاملB -B0-Mixing with Domain-Wall Light Quarks and Relativistic Heavy Quarks
We propose a precise determination of the B-B0 mixing matrix elements and their ratio, ξ ≡ fBs √
متن کاملSemileptonic and Rare B-Meson Transitions in a QCD Relativistic Potential Model
Using a QCD relativistic potential model, previously applied to the calculation of the heavy meson leptonic constants, we evaluate the form factors governing the exclusive decays B → ρ`ν, B → Kγ and B → K``. In our approach the heavy meson is described as a Qq bound state, whose wave function is solution of the relativistic Salpeter equation, with an instantaneous potential displaying Coulombic...
متن کاملEffects of final state interaction in B^+_c to D^0 K^+ decay
In this paper, the decay of Bc+ meson, which consists of two b and c heavy quarks, into the Do and K+ mesons was studied. Given that the experimental branching ratio for this decay was within the range of 3.75*10-5 to 11.16*10-5; it was decided to calculate the theoretical branching ratio by applying the final state interaction (FSI) through the T and cross-section channels. In this process, b...
متن کامل