We use a global fit to determine the form factor slopes and branching fractions of the decays B → Dν and B → D∗ν. We reconstruct D pairs and con-struct a 3-dimensional distribution binned in lepton momentum, D momentum and cosΘB−D. These kinematic variables provide good separation between the signal and background. We fit electron and muon samples separately and combine them after calculating systematic uncertainties. The form factor slopes, ρ2D for B → Dν and ρ2 for B → D∗ν decays, are measured to be ρ2D = 1.22 ± 0.04 ± 0.07 and ρ2 = 1.21 ± 0.02 ± 0.07, where the errors are statistical and systematic, respectively. Branching fractions are fitted to be B(B+ → D̄0+ν) = (2.36 ± 0.03 ± 0.12) % and B(B+ → D̄∗0+ν) = (5.37 ± 0.02 ± 0.21) %. W...
We report the results of a study of the exclusive charmless semileptonic decays, B[superscript +]→η[...
We report the results of a study of the exclusive charmless semileptonic decays, B0→π−ℓ+ν, B+→π0ℓ+ν,...
Semileptonic ¯¯¯ B decays to D X ℓ ¯ ν ( ℓ = e or μ ) are selected by reconstructing D 0 ℓ and D + ℓ...
Based on a sample of 500 million e+e−→cc¯ events recorded by the BaBar detector at c.m. energies of ...
Based on a sample of 500 million e+e-→cc¯ events recorded by the BABAR detector at c.m. energies of ...
Based on a sample of 500 million e+e-→cc¯ events recorded by the BABAR detector at c.m. energies of ...
28 pages, 15 postscript figures, submitted to Phys.Rev.D - See paper for full list of authorsInterna...
Using a sample of 3.3 × 10 B-meson decays collected with the CLEO detector at the Cornell Electron ...
We have studied the decayB →Dlν where l = e or μ. From a fit to the differential decay ratedγ/dwwe ...
We present measurements of the branching fractions for the three-body decays B 0 → D ( * ) ∓ K 0 π ±...
We report the results of a study of the exclusive charmless semileptonic decays, B0→π -+ν, B +→π0 +ν...
We present a combined measurement of the Cabibbo-Kobayashi-Maskawa matrix element | V c b | and of t...
We report the results of a study of the exclusive charmless semileptonic decays, B0\u2192\u3c0 -+\u3...
Semileptonic B̅ decays to DXℓν̅ (ℓ=e or μ) are selected by reconstructing D0ℓ and D+ℓ combinations f...
We present a combined measurement of the Cabibbo-Kobayashi-Maskawa matrix element |Vcb| and of the p...
We report the results of a study of the exclusive charmless semileptonic decays, B[superscript +]→η[...
We report the results of a study of the exclusive charmless semileptonic decays, B0→π−ℓ+ν, B+→π0ℓ+ν,...
Semileptonic ¯¯¯ B decays to D X ℓ ¯ ν ( ℓ = e or μ ) are selected by reconstructing D 0 ℓ and D + ℓ...
Based on a sample of 500 million e+e−→cc¯ events recorded by the BaBar detector at c.m. energies of ...
Based on a sample of 500 million e+e-→cc¯ events recorded by the BABAR detector at c.m. energies of ...
Based on a sample of 500 million e+e-→cc¯ events recorded by the BABAR detector at c.m. energies of ...
28 pages, 15 postscript figures, submitted to Phys.Rev.D - See paper for full list of authorsInterna...
Using a sample of 3.3 × 10 B-meson decays collected with the CLEO detector at the Cornell Electron ...
We have studied the decayB →Dlν where l = e or μ. From a fit to the differential decay ratedγ/dwwe ...
We present measurements of the branching fractions for the three-body decays B 0 → D ( * ) ∓ K 0 π ±...
We report the results of a study of the exclusive charmless semileptonic decays, B0→π -+ν, B +→π0 +ν...
We present a combined measurement of the Cabibbo-Kobayashi-Maskawa matrix element | V c b | and of t...
We report the results of a study of the exclusive charmless semileptonic decays, B0\u2192\u3c0 -+\u3...
Semileptonic B̅ decays to DXℓν̅ (ℓ=e or μ) are selected by reconstructing D0ℓ and D+ℓ combinations f...
We present a combined measurement of the Cabibbo-Kobayashi-Maskawa matrix element |Vcb| and of the p...
We report the results of a study of the exclusive charmless semileptonic decays, B[superscript +]→η[...
We report the results of a study of the exclusive charmless semileptonic decays, B0→π−ℓ+ν, B+→π0ℓ+ν,...
Semileptonic ¯¯¯ B decays to D X ℓ ¯ ν ( ℓ = e or μ ) are selected by reconstructing D 0 ℓ and D + ℓ...