Lattice Results for Heavy Light Matrix Elements

نویسنده

  • A. Soni
چکیده

Lattice results for heavy light matrix elements are reviewed and some of their implications are very briefly discussed [1]. Despite the fact that in most cases the lattice results for weak matrix elements at the moment have only a modest accuracy of about 20–30% they already have important phenomenological repercussions; e.g. for Vtd/Vts, xs/xd and B → K ∗γ. I. As samples of “new” projects, I briefly discuss four projects a. The NRQCD group [2] reports a preliminary result on the mass splitting mB∗ S −mBS . They use 100 configurations on a 16 × 32 lattice of the HEMCGC group (dynamical, staggered nf = 2, am = .01 and β = 5.6). Their very preliminary result is mB∗ S −mBS = [50± 5(statistical)± 10(am) ±15(scale)]MeV (1) Since rough phenomenological estimates for the splitting invariable yield about 50 MeV, such a lattice calculation will be very interesting if the errors can be brought down to 0 (5 MeV). b. The LANL collaboration [3] is acquiring many interesting results via their large scale simulations on the CM-5. So far they have analyzed 58 configurations of size 32 × 64 at β = 6.0. This lattice has the distinction of having the largest physical volume used so far for weak matrix element calculations. Comparison with results previously obtained on smaller lattices will therefore be very valuable. Here are some of their preliminary findings: (1) fK/fπ = 1.163± .023; (2) f + (q =0) f + (q2=0) = 0.86± .08; (2) (3) A ∗ eν 2 (0) A eν 1 (0) = .77± .22. c. The Fermilab Static Group (FSG) [4] is now finishing a comprehensive study with the use of their static method. They reported interesting results on fB, fBS/fBu andmBS−mBu . With their method they find a significant lattice spacing (a) dependence for fB whereas the other two quantities appear insensitive to a. Their key results are: fB = 188± 23(stat)± 15(sys) +27 −0 (extr)± 14(a) (3) fBS/fBu = 1.216± .041± .016 (4) mBS −mBu = 86± 12± 7(MeV) (5) d. MILC collaboration [5] is undertaking a dedicated study of fB using primarily the Intel Paragon machine. They have analyzed so far 40 configurations (24 × 80, β = 6.3). Their preliminary results for the decay constants are given below: fB = 174± 7 MeV fBS = 198± 7 MeV fD = 205± 5 MeV (6) fDS = 228± 5 MeV

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Semileptonic decay of a heavy-light pseudoscalar to a light vector meson

Semileptonic decays of heavy-light mesons are of interest because they can be used to determine elements of the CKM matrix. The nonperturbative QCD information needed to understand a decay can be calculated in lattice QCD. In the case of the decays D → K∗ and Ds → φ the branching ratios have been accurately measured and the relevant CKM matrix element (Vcs) is well determined by other methods [...

متن کامل

Status and Prospects for Lattice Calculations in Heavy Quark Physics

The current status of lattice calculation of weak matrix elements for heavy quark systems is reviewed. After an assessment of systematic errors in present simulations, results for the B meson decay constant, the B parameter BB and semi-leptonic heavy-to-light and heavy-to-heavy transitions are discussed. The final topic are lattice results for heavy baryon spectroscopy.

متن کامل

Point-Split Lattice Operators for B Decays

The matrix element which determines the B meson decay constant can be measured on the lattice using an effective field theory for heavy quarks. Various discretizations of the heavy-light bilinears which appear in this and other B decay matrix elements are possible. The heavy-light bilinear currently used for the determination of the B meson decay constant on the lattice suffers a substantial on...

متن کامل

Matrix elements of heavy - light mesons from a fine lattice

We performed a calculation of matrix elements of heavy mesons on a quenched lattice, generated with Wilson gauge fields at β = 6.6 with a lattice size of 403 ×80 and a lattice spacing a−1 ≃ 5 GeV determined from the Sommer parameter r0 = 0.5 fm. We use a non-perturbatively O(a) improved Wilson fermion action and improved currents. We have calculated the charmonium spectrum as well as form facto...

متن کامل

Matrix elements of four-fermion operators in the HQET

The B-B̄ mixing, B-meson lifetimes, the Bs-B̄s lifetime difference and SUSY FCNC effects in ∆B = 2 processes are very important measurable quantities in B-meson phenomenology whose theoretical predictions depend on unknown matrix elements of several four–fermion operators. We present preliminary results for the matrix elements of the relevant four–fermion operators computed on a sample of 600 lat...

متن کامل

Tadpole-improved perturbation theory for heavy-light lattice operators.

Lattice calculations of matrix elements involving heavy-light quark bilinears are of interest in calculating a variety of properties of B and D mesons, including decay constants and mixing parameters. A large source of uncertainty in the determination of these properties has been uncertainty in the normalization of the lattice-regularized operators that appear in the matrix elements. Tadpole-im...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 1994