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  4. Measurement of CP violation observables and parameters for the decays B[superscript ±]→DK[superscript *±]

Measurement of CP violation observables and parameters for the decays B[superscript ±]→DK[superscript *±]

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Author(s)
Dujmic, Denis
•
Henderson, Shawn Wesley
•
Sciolla, Gabriella
•
Fisher, Peter H
•
Spitznagel, Michael A
•
Yamamoto, R. K.
•
Zhao, M.
•
Cowan, Ray F
Alternative Title
Measurement of CP violation observables and parameters for the decays B±→DK*±
Date Issued
November 2009
Journal
Physical Review D
Publisher
American Physical Society
Citation
Aubert, B. et al. “Measurement of CP violation observables and parameters for the decays B±-->DK*±.” Physical Review D 80.9 (2009): 092001. © 2009 The American Physical Society
Version
Final published version
Abstract
We study the decay B[superscript -]→DK[superscript *-] using a sample of 379×10[superscript 6] Υ(4S)→BB̅ events collected with the BABAR detector at the PEP-II B factory. We perform a Gronau-London-Wyler analysis where the D meson decays into either a CP-even (CP+) eigenstate (K[superscript +]K[superscript -], π[superscript +]π[superscript -]), CP-odd (CP-) eigenstate (KS[superscript 0]π[superscript 0], K[subscript S][superscript 0]ϕ, K[subscript S][superscript 0]ω) or a non-CP state (K[superscript -]πsuperscript +]). We also analyze D meson decays into Ksuperscript +]πsuperscript -] from a Cabibbo-favored D̅ 0 decay or doubly suppressed D0 decay [Atwood-Dunietz-Soni (ADS) analysis]. We measure observables that are sensitive to the Cabibbo-Kobayashi-Maskawa angle γ: the partial-rate charge asymmetries A[subscript CP±], the ratios R[subscript CP±] of the B-decay branching fractions in CP± and non-CP decay, the ratio R[subscript ADS] of the charge-averaged branching fractions, and the charge asymmetry A[subscript ADS] of the ADS decays: A[subscript CP+]=0.09±0.13±0.06, A[subscript CP-]=-0.23±0.21±0.07, R[subscript CP+]=2.17±0.35±0.09, R[subscript CP-]=1.03±0.27±0.13, R[subscript ADS]=0.066±0.031±0.010, and A[subscript ADS]=-0.34±0.43±0.16, where the first uncertainty is statistical and the second is systematic. Combining all the measurements and using a frequentist approach yields the magnitude of the ratio between the Cabibbo-suppressed and favored amplitudes, r[subscript B]=0.31 with a one (two) sigma confidence level interval of [0.24, 0.38] ([0.17, 0.43]). The value r[subscript B]=0 is excluded at the 3.3 sigma level. A similar analysis excludes values of γ in the intervals [0, 7]°, [55, 111]°, and [175, 180]° ([85, 99]°) at the one (two) sigma confidence level.
MIT Department
Massachusetts Institute of Technology. Department of Physics
Massachusetts Institute of Technology. Laboratory for Nuclear Science
Terms of Use
Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use.
Persistent DSpace Link
http://hdl.handle.net/1721.1/56294
DOI of Published Version
http://dx.doi.org/10.1103/PhysRevD.80.092001
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