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Observation of B+ ---> a(1)+(1260) K0 and B0 ---> a(1)-(1260) K+
No full textWe present branching fraction measurements of the decays B^{+} -> a1(1260)^{+} K^{0} and B^{0} to a1(1260)^{-} K^{+} with a1(1260)^{+} -> pi^{-} pi^{+} pi^{+}. The data sample corresponds to 383 million B B-bar pairs produced in e^{+}e^{-} annihilation through the Y(4S) resonance. We measure the products of the branching fractions:
B(B^{+}-> a1(1260)^{+} K^{0})B(a1(1260)^{+} -> pi^{-} pi^{+} pi^{+}) = (17.4 +/- 2.5 +/- 2.2) 10^{-6}
B(B^{0}-> a1(1260)^{-} K^{+})B(a1(1260)^{-} -> pi^{+} pi^{-} pi^{-}) = (8.2 +/- 1.5 +/- 1.2) 10^{-6}.
We also measure the charge asymmetries A_{ch}(B^{+} -> a1(1260)^{+} K^{0})= 0.12 +/- 0.11 +/- 0.02 and A_{ch}(B^{0} -> a1(1260)^{-} K^{+})= -0.16 +/- 0.12 +/- 0.01. The first uncertainty quoted is statistical and the second is systematic
Observation of B+→a1+(1260)K0 and B0→a1-(1260)K+
Full text linkWe present branching fraction measurements of the decays B+→a1+(1260)K0 and B0→a1-(1260)K+ with a1±(1260)→π∓π±π±. The data sample corresponds to 383×106 BB̅ pairs produced in e+e- annihilation through the Υ(4S) resonance. We measure the products of the branching fractions B(B+→a1+(1260)K0)B(a1+(1260)→π-π+π+)=(17.4±2.5±2.2)×10-6 and B(B0→a1-(1260)K+)B(a1-(1260)→π+π-π-)=(8.2±1.5±1.2)×10-6. We also measure the charge asymmetries Ach(B+→a1+(1260)K0)=0.12±0.11±0.02 and Ach(B0→a1-(1260)K+)=-0.16±0.12±0.01. The first uncertainty quoted is statistical and the second is systematic
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Observation of B+-->a1+(1260)K0 and B0-->a1-(1260)K+.
Full text linkWe present branching fraction measurements of the decays B(+)-->a(1)(+)(1260)K(0) and B(0)-->a(1)(-)(1260)K(+) with a(1)(+/-)(1260)-->pi(-/+)pi(+/-)pi(+/-). The data sample corresponds to 383 x 10(6) BB pairs produced in e(+)e(-) annihilation through the Upsilon(4S) resonance. We measure the products of the branching fractions B(B(+)-->a(1)(+)(1260)K(0)B(a(1)(+)(1260)-->pi(-)pi(+)pi(+))=(17.4+/-2.5+/-2.2) x 10(-6) and B(B(0)-->a(1)(-)(1260)K(+)B(a(1)(-)(1260)-->pi(+)pi(-)pi(-)) = (8.2+/-1.5+/-1.2) x 10(-6). We also measure the charge asymmetries A(ch)(B(+)-->a(1)(+)(1260)K(0) = 0.12+/-0.11+/-0.02 and A(ch)(B(0)-->a(1)(-)(1260)K+) = -0.16+/-0.12+/-0.01. The first uncertainty quoted is statistical and the second is systematic
Observation of B+→a1+(1260)K0 and B0→a1-(1260)K+
No full textWe present branching fraction measurements of the decays B+→a1+(1260)K0 and B0→a1-(1260)K+ with a1±(1260)→π∓π±π±. The data sample corresponds to 383×106 BB̅ pairs produced in e+e- annihilation through the Υ(4S) resonance. We measure the products of the branching fractions B(B+→a1+(1260)K0)B(a1+(1260)→π-π+π+)=(17.4±2.5±2.2)×10-6 and B(B0→a1-(1260)K+)B(a1-(1260)→π+π-π-)=(8.2±1.5±1.2)×10-6. We also measure the charge asymmetries Ach(B+→a1+(1260)K0)=0.12±0.11±0.02 and Ach(B0→a1-(1260)K+)=-0.16±0.12±0.01. The first uncertainty quoted is statistical and the second is systematic
Observation of B+→a+1(1260)K0 and B0→a−1(1260)K+
No full textWe present branching fraction measurements of the decays B + → a + 1 ( 1260 ) K 0 and B 0 → a − 1 ( 1260 ) K + with a ± 1 ( 1260 ) → π ∓ π ± π ± . The data sample corresponds to 383 × 10 6 B ¯¯¯ B pairs produced in e + e − annihilation through the Υ ( 4 S ) resonance. We measure the products of the branching fractions B ( B + → a + 1 ( 1260 ) K 0 ) B ( a + 1 ( 1260 ) → π − π + π + ) = ( 17.4 ± 2.5 ± 2.2 ) × 10 − 6 and B ( B 0 → a − 1 ( 1260 ) K + ) B ( a − 1 ( 1260 ) → π + π − π − ) = ( 8.2 ± 1.5 ± 1.2 ) × 10 − 6 . We also measure the charge asymmetries A ch ( B + → a + 1 ( 1260 ) K 0 ) = 0.12 ± 0.11 ± 0.02 and A ch ( B 0 → a − 1 ( 1260 ) K + ) = − 0.16 ± 0.12 ± 0.01 . The first uncertainty quoted is statistical and the second is systematic
Observation and polarization measurement of B^{0}→a_{1}(1260)^{+}a_{1}(1260)^{-} decay
Full text linkWe present measurements of the branching fraction B and longitudinal polarization fraction fL for B0→a1(1260)+a1(1260)- decays, with a1(1260)±→π-π+π±. The data sample, collected with the BABAR detector at the SLAC National Accelerator Laboratory, represents 465×106 produced BB̅ pairs. We measure B(B0→a1(1260)+a1(1260)-)×[B(a1(1260)+→π-π+π+)]2= (11.8±2.6±1.6)×10-6 and fL=0.31±0.22±0.10, where the first uncertainty is statistical and the second systematic. The decay mode is measured with a significance of 5.0 standard deviations including systematic uncertainties
Observation and polarization measurement of B^0 → a_1(1260)^(+)a_1(1260)^(-) decay
Full text linkWe present measurements of the branching fraction B and longitudinal polarization fraction f_L for B^0 → a_1(1260)^(+)a_1(1260)^(-) decays, with a_1(1260)^(±) → π^(-)π^(+)π^(±). The data sample, collected with the BABAR detector at the SLAC National Accelerator Laboratory, represents 465 × 10^6 produced BB(overbar) pairs. We measure B(B^0 → a_1(1260)^(+)a_1(1260)^-) × [B(a_1(1260)^+ → π^(-)π^(+)π^(+))]^2 = (11.8±2.6±1.6) ×10^(-6) and f_L = 0.31±0.22±0.10, where the first uncertainty is statistical and the second systematic. The decay mode is measured with a significance of 5.0 standard deviations including systematic uncertainties
Observation and polarization measurement of B0→a1(1260)+a1(1260)− decay
No full textWe present measurements of the branching fraction B and longitudinal polarization fraction f L for B 0 → a 1 ( 1260 ) + a 1 ( 1260 ) − decays, with a 1 ( 1260 ) ± → π − π + π ± . The data sample, collected with the BABAR detector at the SLAC National Accelerator Laboratory, represents 465 × 10 6 produced B ¯¯¯ B pairs. We measure B ( B 0 → a 1 ( 1260 ) + a 1 ( 1260 ) − ) × [ B ( a 1 ( 1260 ) + → π − π + π + ) ] 2 = ( 11.8 ± 2.6 ± 1.6 ) × 10 − 6 and f L = 0.31 ± 0.22 ± 0.10 , where the first uncertainty is statistical and the second systematic. The decay mode is measured with a significance of 5.0 standard deviations including systematic uncertainties
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