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Observation of B0 Meson Decays to A1(1260)+- Pi-

Observation of B0 Meson Decays to A1(1260)+- Pi-
Author: B. Aubert
Publisher:
Total Pages: 7
Release: 2006
Genre:
ISBN:

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The authors present a measurement of the branching fraction of the decay B{sup 0} {yields} a{sub 1}{sup {+-}}(1260){pi}{sup {-+}} with a{sub 1}{sup {+-}}(1260) {yields} {pi}{sup {-+}}{pi}{sup {+-}}{pi}{sup {+-}}. The data sample corresponds to 218 x 10{sup 6} B{bar B} pairs produced in e{sup +}e{sup -} annihilation through the {Upsilon}(4S) resonance. The authors measure the branching fraction {Beta}(B{sup 0} {yields} a{sub 1}{sup {+-}}(1260){pi}{sup {-+}}){Beta}(a{sub 1}{sup {+-}}(1260){yields} {pi}{sup {-+}}{pi}{sup {+-}}{pi}{sup {+-}})=(16.6 {+-} 1.9 {+-} 1.5) x 10{sup -6}, where the first error quoted is statistical and the second is systematic.


Observation of B Meson Decays to Eta Pi and Eta K.

Observation of B Meson Decays to Eta Pi and Eta K.
Author:
Publisher:
Total Pages: 18
Release: 2003
Genre:
ISBN:

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The authors present preliminary measurements of the B meson decays B 2![eta][pi], B+ 2![eta]K+, and B° 2![eta]K°. The data were recorded with the BABAR detector at PEP II and correspond to 88.9 x 106 B{bar B} pairs produced in e+e− annihilation through the [Upsilon](4S) resonance. They find the branching fractions [Beta](B+ 2![eta][pi]+) = (4.2{sub -0.9}{sup +1.0} ± 0.3) x 10−6 and [Beta](B+ 2![eta]K+) = (2.8{sub -0.7}{sup +0.8} ± 0.2) x 10−6. They set a 90% CL upper limit of [Beta](B° 2![eta]K°)


Observation of B[sup 0] Meson Decay to [alpha][sub 1][sup +](1260) [pi][sup -].

Observation of B[sup 0] Meson Decay to [alpha][sub 1][sup +](1260) [pi][sup -].
Author:
Publisher:
Total Pages:
Release: 2004
Genre:
ISBN:

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The authors present a preliminary measurement of the branching fraction of the B meson decay B[sup 0] --> [alpha][sup 1][sup +](1260) --> [pi][sup +][pi][sup +][pi][sup -]. The data were recorded with the BABAR detector at the SLAC B factory PEP-II and correspond to 124 x 10[sup 6] B[bar B] pairs produced in e[sup +]e[sup -] annihilation through the [Upsilon](4S) resonance. They find the branching fraction B(B[sup 0] --> [alpha][sub 1][sup +](1260)[pi][sup -]) = (42.6 [+-] 4.2 [+-] 4.1) x 10[sup -6]. The fitted values of the [alpha][sub 1](1260) parameters are m[sub [alpha][sub 1]] = 1.19 [+-] 0.02 GeV/c[sup 2] and [Gamma][sub [alpha][sub 1]] = 312 [+-] 55 MeV/c[sup 2].


Study of B Meson Decays to Ppbarh Final States

Study of B Meson Decays to Ppbarh Final States
Author: Tetiana B. Hryn'ova
Publisher:
Total Pages: 165
Release: 2006
Genre:
ISBN:

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B mesons are unique among well-established non-quarkonium mesons in their ability to decay into baryons. Baryonic B decays offer a wide range of interesting areas of study: they can be used to test our theoretical understanding of rare decay processes involving baryons, search for direct CP violation and study low-energy QCD. This thesis presents measurements of branching fractions and a study of the decay dynamics of the charmless three-body decays of B meson into p{bar p}h final states, where h = {pi}{sup +}, K{sup +}, K{sub S}{sup 0}, K*{sup 0} or K*{sup +}. With a sample of 232 million {Upsilon}(4S) {yields} B{bar B} events collected with the BaBar detector, we report the first observation of the B {yields} p{bar p}K*{sup 0} decay, and provide improved measurements of branching fractions of the other modes. The distribution of the three final-state particles is of particular interest since it provides dynamical information on the possible presence of exotic intermediate states such as the hypothetical pentaquark states {Theta}*{sup ++} and {Theta}{sup +}in the m{sub pK{sup +}} and m{sub pK{sub S}{sup 0}} spectra, respectively, or glueball states (such as the tensor glueball f{sub J}(2220)) in the m{sub p{bar p}} spectrum. No evidence for exotic states is found and upper limits on the branching fractions are set. An enhancement at low p{bar p} mass is observed in all the B {yields} p{bar p}h modes, and its shape is compared between the decay modes and with the shape of the time-like proton form factor. A Dalitz plot asymmetry in B {yields} p{bar p}K{sup +} mode suggests dominance of the penguin amplitude in this decay and disfavors the possibility that the low mass p{bar p} enhancement originates from the presence of a resonance below threshold (such as the recently seen baryonium candidate at 1835 MeV/c{sup 2}). We also identify decays of the type B {yields} X{sub c{bar c}}h {yields} p{bar p}h, where h = K{sup +}, K{sub S}{sup 0}, K*{sup 0} or K*{sup +}, and X{sub c{bar c}} = {eta}{sub c} or J/{psi}. In particular, we report on the evidence of the B {yields} {eta}{sub c}K*{sup +} decay and provide a measurement of the width of {eta}{sub c}.


Observation of B Meson Decays to Omegapi+, OmegaK+, and OmegaK0

Observation of B Meson Decays to Omegapi+, OmegaK+, and OmegaK0
Author:
Publisher:
Total Pages: 15
Release: 2003
Genre:
ISBN:

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The authors present preliminary measurements of B meson decays to B 2![omega][pi], B+ 2![omega]K+, and B° 2![omega]K°. The data were recorded with the BABAR detector and correspond to 88.9 x 106 B{bar B} pairs produced in e+e− annihilation at the [Upsilon](4S) resonance. They find statistically significant signals for all three channels: [Beta](B+ 2![omega][pi]+) = (5.4 ± 1.0 ± 0.5) x 10−6, [Beta](B+ 2![omega]K+) = (5.0 ± 1.0 ± 0.4) x 10−6, and [Beta](B° 2![omega]K°) = (5.3{sub -1.2}{sup +1.4} ± 0.5) x 10−6. They also measure time-integrated charge asymmetries [Alpha]{sub ch}(B+ 2![omega][pi]+) = 0.04 ± 0.17 ± 0.01 and [Alpha]{sub ch}(B+ 2![omega]K+) = -0.05 ± 0.16 ± 0.01.