We present measurements of the semileptonic decays B-→D0τ-ν̅ τ, B-→D*0τ-ν̅ τ, B̅ 0→D+τ-ν̅ τ, and B̅ 0→D*+τ-ν̅ τ, which are sensitive to non-standard model amplitudes in certain scenarios. The data sample consists of 232×106 Υ(4S)→BB̅ decays collected with the BABAR detector at the PEP-II e+e- collider. We select events with a D or D* meson and a light lepton (ℓ=e or μ) recoiling against a fully reconstructed B meson. We perform a fit to the joint distribution of lepton momentum and missing mass squared to distinguish signal B̅ →D(*)τ-ν̅ τ(τ-→ℓ-ν̅ ℓντ) events from the backgrounds, predominantly B̅ →D(*)ℓ-ν̅ ℓ. We measure the branching-fraction ratios R(D)≡B(B̅ →Dτ-ν̅ τ)/B(B̅ →Dℓ-ν̅ ℓ) and R(D*)≡B(B̅ →D*τ-ν̅ τ)/B(B̅ →D*ℓ-ν̅ ℓ) and, from a co...
Semileptonic B̅ decays to DXlν̅ (l=e or μ) are selected by reconstructing D0l and D+l combinations f...
We report on measurements of the decays of B¯ mesons into the semileptonic final states B¯→D(∗)π+π-ν...
Semileptonic B̅ decays to DXℓν̅ (ℓ=e or μ) are selected by reconstructing D0ℓ and D+ℓ combinations...
We present measurements of the semileptonic decays B-→D0τ- ν̄τ, B-→D*0τ-ν̄τ, B̄0→D+τ- ν̄τ, and B̄0→D...
We present measurements of the semileptonic decays B-\u2192D0\u3c4-\u3bd\u305 \u3c4, B-\u2192D*0\u3c...
We present measurements of the semileptonic decays B − → D 0 τ − ¯ ν τ , B − → D * 0 τ − ¯ ν τ , ¯¯¯...
We present measurements of the semileptonic decays B-→D0τ- ν̄τ, B-→D*0τ-ν̄τ, B̄0→D+τ- ν̄τ, and B̄0→D...
We present measurements of the semileptonic decays B − → D 0 τ − ¯ ν τ , B − → D * 0 τ − ¯ ν τ , ¯¯¯...
We present measurements of the semileptonic decays B-→D0τ-ν̅ τ, B-→D*0τ-ν̅ τ, B̅ 0→D+τ-ν̅ τ, and B̅ ...
We present measurements of the semileptonic decays B-\u2192D0\u3c4-\u3bd\u305 \u3c4, B-\u2192D*0\u3c...
Semileptonic B̄ decays to DXν̄ (=e or μ) are selected by reconstructing D0 and D+ combinations from ...
Semileptonic B̄ decays to DXν̄ (=e or μ) are selected by reconstructing D0 ; D+ combinations from a ...
We present measurements of the semileptonic decays B--->D0tau-nutau, B--->D*0tau-nutau, B0--&g...
We report on measurements of the decays of B¯ mesons into the semileptonic final states B¯→D^(*)π^(+...
We report on measurements of the decays of B¯ mesons into the semileptonic final states B¯→D^(*)π^(+...
Semileptonic B̅ decays to DXlν̅ (l=e or μ) are selected by reconstructing D0l and D+l combinations f...
We report on measurements of the decays of B¯ mesons into the semileptonic final states B¯→D(∗)π+π-ν...
Semileptonic B̅ decays to DXℓν̅ (ℓ=e or μ) are selected by reconstructing D0ℓ and D+ℓ combinations...
We present measurements of the semileptonic decays B-→D0τ- ν̄τ, B-→D*0τ-ν̄τ, B̄0→D+τ- ν̄τ, and B̄0→D...
We present measurements of the semileptonic decays B-\u2192D0\u3c4-\u3bd\u305 \u3c4, B-\u2192D*0\u3c...
We present measurements of the semileptonic decays B − → D 0 τ − ¯ ν τ , B − → D * 0 τ − ¯ ν τ , ¯¯¯...
We present measurements of the semileptonic decays B-→D0τ- ν̄τ, B-→D*0τ-ν̄τ, B̄0→D+τ- ν̄τ, and B̄0→D...
We present measurements of the semileptonic decays B − → D 0 τ − ¯ ν τ , B − → D * 0 τ − ¯ ν τ , ¯¯¯...
We present measurements of the semileptonic decays B-→D0τ-ν̅ τ, B-→D*0τ-ν̅ τ, B̅ 0→D+τ-ν̅ τ, and B̅ ...
We present measurements of the semileptonic decays B-\u2192D0\u3c4-\u3bd\u305 \u3c4, B-\u2192D*0\u3c...
Semileptonic B̄ decays to DXν̄ (=e or μ) are selected by reconstructing D0 and D+ combinations from ...
Semileptonic B̄ decays to DXν̄ (=e or μ) are selected by reconstructing D0 ; D+ combinations from a ...
We present measurements of the semileptonic decays B--->D0tau-nutau, B--->D*0tau-nutau, B0--&g...
We report on measurements of the decays of B¯ mesons into the semileptonic final states B¯→D^(*)π^(+...
We report on measurements of the decays of B¯ mesons into the semileptonic final states B¯→D^(*)π^(+...
Semileptonic B̅ decays to DXlν̅ (l=e or μ) are selected by reconstructing D0l and D+l combinations f...
We report on measurements of the decays of B¯ mesons into the semileptonic final states B¯→D(∗)π+π-ν...
Semileptonic B̅ decays to DXℓν̅ (ℓ=e or μ) are selected by reconstructing D0ℓ and D+ℓ combinations...