Author/Authors :
OPAL Collaboration، نويسنده , , G. Abbiendi، نويسنده , , K. Ackerstaff، نويسنده , , P.F. Akesson، نويسنده , , G. Alexander، نويسنده , , J. Allison، نويسنده , , K.J. Anderson، نويسنده , , S. Arcelli، نويسنده , , S. Asai، نويسنده , , S.F Ashby، نويسنده , , D. Axen، نويسنده , , G. Azuelos، نويسنده , , I. Bailey، نويسنده , , A.H. Ball، نويسنده , , E. Barberio، نويسنده , , R.J. Barlow، نويسنده , , J.R. Batley، نويسنده , , Leslie S. Baumann، نويسنده , , T. Behnke، نويسنده , , K.W. Bell، نويسنده , , et al.، نويسنده ,
Abstract :
The magnitude of the Cabibbo-Kobayashi-Maskawa matrix element Vcb has been measured using B̄0→D∗+ℓ−ν̄ decays recorded on the Z0 peak using the OPAL detector at LEP. The D∗+→D0π+ decays were reconstructed both in the particular decay modes D0→K−π+ and D0→K−π+π0 and via an inclusive technique. The product of |Vcb| and the decay form factor of the B̄0→D∗+ℓ−ν̄ transition at zero recoil F(1) was measured to be F(1)|Vcb|=(37.1±1.0±2.0)×10−3, where the uncertainties are statistical and systematic respectively. By using Heavy Quark Effective Theory calculations for F(1), a value of|Vcb|=(40.7±1.1±2.2±1.6)×10−3was obtained, where the third error is due to theoretical uncertainties in the value of F(1). The branching ratio Br(B̄0→D∗+ℓ−ν̄) was also measured to be (5.26±0.20±0.46)%.
