Observation of B(0) --> D0pi(0) and B(0) -->D(*0)pi(0).

We have studied the color-suppressed hadronic decays of neutral B mesons into the final states D*0pi(0). Using 9.67 x 10(6) BB pairs collected with the CLEO detector, we observe the decays B( 0) --> D0pi(0) and B( 0) -->D(*0)pi(0) with the branching fractions BB( 0) -->D0pi(0))...

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Κύριοι συγγραφείς: Coan, T, Gao, Y, Liu, F, Maravin, Y, Narsky, I, Stroynowski, R, Ye, J, Artuso, M, Boulahouache, C, Bukin, K, Dambasuren, E, Mountain, R, Skwarnicki, T, Stone, S, Wang, J, Mahmood, A, Csorna, SE, Danko, I, Xu, Z, Bonvicini, G, Cinabro, D, Dubrovin, M, McGee, S, Bornheim, A, Lipeles, E
Μορφή: Journal article
Γλώσσα:English
Έκδοση: 2002
_version_ 1826294020746248192
author Coan, T
Gao, Y
Liu, F
Maravin, Y
Narsky, I
Stroynowski, R
Ye, J
Artuso, M
Boulahouache, C
Bukin, K
Dambasuren, E
Mountain, R
Skwarnicki, T
Stone, S
Wang, J
Mahmood, A
Csorna, SE
Danko, I
Xu, Z
Bonvicini, G
Cinabro, D
Dubrovin, M
McGee, S
Bornheim, A
Lipeles, E
author_facet Coan, T
Gao, Y
Liu, F
Maravin, Y
Narsky, I
Stroynowski, R
Ye, J
Artuso, M
Boulahouache, C
Bukin, K
Dambasuren, E
Mountain, R
Skwarnicki, T
Stone, S
Wang, J
Mahmood, A
Csorna, SE
Danko, I
Xu, Z
Bonvicini, G
Cinabro, D
Dubrovin, M
McGee, S
Bornheim, A
Lipeles, E
author_sort Coan, T
collection OXFORD
description We have studied the color-suppressed hadronic decays of neutral B mesons into the final states D*0pi(0). Using 9.67 x 10(6) BB pairs collected with the CLEO detector, we observe the decays B( 0) --> D0pi(0) and B( 0) -->D(*0)pi(0) with the branching fractions BB( 0) -->D0pi(0)) = (2.74(+0.36)(-0.32) +/- 0.55)x10(-4) and BB( 0) -->D(*0)pi(0)) = (2.20(+0.59)(-0.52) +/- 0.79)x10(-4). The first error is statistical and the second systematic. The statistical significance of the D0pi(0) signal is 12.1sigma ( 5.9sigma for D(*0)pi(0)). Utilizing the B( 0) -->D*0)pi(0) branching fractions we determine the strong phases delta(I,D(*)) between isospin 1/2 and 3/2 amplitudes in the Dpi and D*pi final states to be cosdelta(I,D) = 0.89 +/-0.08 and cosdelta(I,D*) = 0.89 +/- 0.08, respectively.
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spelling oxford-uuid:bd4e140e-7242-499e-b56d-dc5186a305df2022-03-27T05:30:52ZObservation of B(0) --> D0pi(0) and B(0) -->D(*0)pi(0).Journal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:bd4e140e-7242-499e-b56d-dc5186a305dfEnglishSymplectic Elements at Oxford2002Coan, TGao, YLiu, FMaravin, YNarsky, IStroynowski, RYe, JArtuso, MBoulahouache, CBukin, KDambasuren, EMountain, RSkwarnicki, TStone, SWang, JMahmood, ACsorna, SEDanko, IXu, ZBonvicini, GCinabro, DDubrovin, MMcGee, SBornheim, ALipeles, EWe have studied the color-suppressed hadronic decays of neutral B mesons into the final states D*0pi(0). Using 9.67 x 10(6) BB pairs collected with the CLEO detector, we observe the decays B( 0) --> D0pi(0) and B( 0) -->D(*0)pi(0) with the branching fractions BB( 0) -->D0pi(0)) = (2.74(+0.36)(-0.32) +/- 0.55)x10(-4) and BB( 0) -->D(*0)pi(0)) = (2.20(+0.59)(-0.52) +/- 0.79)x10(-4). The first error is statistical and the second systematic. The statistical significance of the D0pi(0) signal is 12.1sigma ( 5.9sigma for D(*0)pi(0)). Utilizing the B( 0) -->D*0)pi(0) branching fractions we determine the strong phases delta(I,D(*)) between isospin 1/2 and 3/2 amplitudes in the Dpi and D*pi final states to be cosdelta(I,D) = 0.89 +/-0.08 and cosdelta(I,D*) = 0.89 +/- 0.08, respectively.
spellingShingle Coan, T
Gao, Y
Liu, F
Maravin, Y
Narsky, I
Stroynowski, R
Ye, J
Artuso, M
Boulahouache, C
Bukin, K
Dambasuren, E
Mountain, R
Skwarnicki, T
Stone, S
Wang, J
Mahmood, A
Csorna, SE
Danko, I
Xu, Z
Bonvicini, G
Cinabro, D
Dubrovin, M
McGee, S
Bornheim, A
Lipeles, E
Observation of B(0) --> D0pi(0) and B(0) -->D(*0)pi(0).
title Observation of B(0) --> D0pi(0) and B(0) -->D(*0)pi(0).
title_full Observation of B(0) --> D0pi(0) and B(0) -->D(*0)pi(0).
title_fullStr Observation of B(0) --> D0pi(0) and B(0) -->D(*0)pi(0).
title_full_unstemmed Observation of B(0) --> D0pi(0) and B(0) -->D(*0)pi(0).
title_short Observation of B(0) --> D0pi(0) and B(0) -->D(*0)pi(0).
title_sort observation of b 0 gt d0pi 0 and b 0 gt d 0 pi 0
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