Abstract

We present measurements of the branching fractions and charge asymmetries (where appropriate) of two-body B decays to η(′)K*, η(′)ρ, η(′)π0, ωπ0, and φπ0. The data were recorded with the BABAR detector at PEP-II and correspond to 89×106 BB¯ pairs produced in e+e− annihilation through the Υ(4S) resonance. We find significant signals for two decay modes and measure the branching fractions B(B+→ηK*+)=(25.6±4.0±2.4)×10−6 and B(B0→ηK*0)=(18.6±2.3±1.2)×10−6, where the first error is statistical and the second systematic. We also find evidence with significance 3.5σ for a third decay mode and measure B(B+→ηρ+)=(9.2±3.4±1.0)×10−6. For other channels, we set 90% C.L. upper limits of B(B0→ηρ0)<1.5×10−6, B(B+→η′K*+)<14×10−6, B(B0→η′K*0)<7.6×10−6, B(B+→η′ρ+)<22×10−6, B(B0→η′ρ0)<4.3×10−6, B(B0→ηπ0)<2.5×10−6, B(B0→η′π0)<3.7×10−6, B(B0→ωπ0)<1.2×10−6, and B(B0→φπ0)<1.0×10−6. For self-flavor-tagging modes with significant signals, the time-integrated charge asymmetries are Ach(ηK*+)=+0.13±0.14±0.02 and Ach(ηK*0)=+0.02±0.11±0.02. Received 17 March 2004DOI:https://doi.org/10.1103/PhysRevD.70.032006©2004 American Physical Society

Highlights

  • We report the results of searches for charged or neutral B-meson decays to the charmless final states1͔ ␩K*, ␩ЈK*, ␩␳, ␩Ј␳, ␩␲0, ␩Ј␲0, ␻␲0, and ␾␲0

  • The results described in this paper complete the measurement of all four (␩,␩Ј)(K,K*) final states, as well as those with (␩,␩Ј)(␲,␳), with a BABAR dataset of 89 million BB decays

  • The results presented in this paper are based on data collected with the BABAR detector18͔ at the PEP-II asymmetric-energy eϩeϪ collider19͔ located at the Stanford Linear Accelerator Center

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Summary

INTRODUCTION

We report the results of searches for charged or neutral B-meson decays to the charmless final states1͔ ␩K*, ␩ЈK*, ␩␳, ␩Ј␳, ␩␲0, ␩Ј␲0, ␻␲0, and ␾␲0. Since the internal tree diagramFig. 2͑b͒ is color-suppressed, the decay is dominated by theexternaltree diagram of Fig. 2͑a. The singlet penguin diagramFig. 3͑e͒ may be significant only for the decays with an ␩Ј in the final state, and the electroweak penguinFig. 3͑f͒ is the only contribution for the B0→␾␲0 decayand negligible for the other decay modes. For B→␩ЈK* the penguin and tree amplitudes are expected to be of similar magnitude, which allows charge asymmetries which could be in the 20– 40 % range5,8,9,11͔. The results described in this paper complete the measurement of all four (␩,␩Ј)(K,K*) final states, as well as those with (␩,␩Ј)(␲,␳), with a BABAR dataset of 89 million BB decays. Results for the final states (␩,␩Ј)(K,␲) on this dataset have been presented elsewhere16,17͔ These data represent an order of magnitude increase in the B meson sample size over the only previous complete study. This ‘‘blind’’ procedure is used to avoid bias in the results

DETECTOR AND DATA
CANDIDATE RECONSTRUCTION AND B MESON SELECTION
Charged track selection
K0 selection
B meson selection
SOURCES OF BACKGROUND AND SUPPRESSION TECHNIQUES
QED and tau-pair backgrounds
QCD continuum backgrounds
BBbackgrounds
MAXIMUM LIKELIHOOD FIT
SIGNAL AND BACKGROUND MODEL
Inclusion of BBbackground in the fits
PDF corrections from data control samples
Fisher parametrization
Pseudoscalar mass parametrization
Vector mass and helicity parametrization
FIT VALIDATION
VIII. EFFICIENCIES AND EFFICIENCY CORRECTIONS
FIT RESULTS
Additive systematic errors
Multiplicative systematic errors
Charge asymmetry systematic errors
COMBINED RESULTS
DISCUSSION
XIII. SUMMARY OF RESULTS
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