Inclusive decays of B-meson to J/ψ and χ c1 using \(\boldsymbol {386\times 10^{6} B\bar {B}}\) events
- 49 Downloads
Abstract
The inclusive decays of B-mesons to charmonium have been studied in a data sample of 386 million \(B\bar {B}\) events. The data sample has been collected by the Belle detector at the KEKB asymmetric energy e + e − collider operating at the Υ(4S) resonance. The branching fractions have been measured for the inclusive decays to J/ψ + X and χ c1 + X. The measured branching fraction for J/ψ + X is \(\mathcal {B}(B \to J/\psi (\to e^{+}e^{-})+X) = (1.10\pm 0.005\pm 0.057)\%\) and \(\mathcal {B}(B\to J/\psi (\to \mu ^{+}\mu ^{-})+X) = (1.08\pm 0.004\pm 0.056)\%\), while the inclusive χ c1 + X branching fraction is found to be \(\mathcal {B}(B\to \chi _{c1}+X) = (0.44\pm 0.01\pm 0.06)\%\). The feed-down contribution from higher charmonium states is subtracted from the measured branching fractions and the direct branching fractions are obtained to be \(\mathcal {B}(B\to J/\psi +X) = (0.77\pm 0.04\pm 0.06)\%\) and \(\mathcal {B}(B \to \chi _{c1}+X) = (0.41\pm 0.01\pm 0.06)\%.\)
Keywords
B-meson CP violation charmonium B-factory Belle detectorPACS Nos
13.25.Hw 11.30.Er 14.40.NdNotes
Acknowledgements
The author is highly grateful to the KEKB group for excellent operation of the accelerator, the KEK cryogenics group for efficient solenoid operations and the KEK computer group and the NII for valuable computing and SINET3 network support. The authors also acknowledge support from MEXT and JSPS (Japan); ARC and DEST (Australia); NSFC (China); DST (India, under Grant No. SR /S2 /HEP-05 /2011); MOEHRD, KOSEF, and KRF (Korea); KBN (Poland); MES and RFAAE (Russia); ARRS (Slovenia); SNSF (Switzerland); NSC and MOE (Taiwan); and DOE (USA).
References
- [1]J J Aubert et al, Phys. Rev. Lett. 33, 1404 (1974)CrossRefADSGoogle Scholar
- [2]J E Augustin et al, Phys. Rev. Lett. 33, 1406 (1974)CrossRefADSGoogle Scholar
- [3]M Neubert and B Stech, Heavy flavours II edited by A J Buras and M Lindner (World Scientific, Singapore, 1988) p. 345Google Scholar
- [4]G T Bodwin, E Braaten, and G P Lepage, Phys. Rev. D 51, 1125 (1995)CrossRefADSGoogle Scholar
- [5]M Beneke, F Maltoni, and I Z Rothstein, Phys. Rev. D 59, 054003 (1999)CrossRefADSGoogle Scholar
- [6]A K Leibovich, Nucl. Phys. Proc. Suppl. 93, 182 (2001)CrossRefADSGoogle Scholar
- [7]BABAR Collaboration: B Aubert et al, Phys. Rev. Lett. 87, 091801 (2001)Google Scholar
- [8]BELLE Collaboration: K Abe et al, Phys. Rev. Lett. 87, 091802 (2001)Google Scholar
- [9]W N Cottingham and D A Greenwood, An introduction to the standard model of particle physics (Cambridge University Press, Cambridge, UK, 1998) p. 1Google Scholar
- [10]S Kurokawa and E Kikutani, Nucl. Instrum. Methods A 499(1), 1 (2003)CrossRefADSGoogle Scholar
- [11]A Abashian et al, Nucl. Instrum. Methods A 479, 117 (2002)CrossRefADSGoogle Scholar
- [12]Belle SVD Group: Y Ushiroda, Nucl. Instrum. Methods A 511, 6 (2003)Google Scholar
- [13]Belle SVD2 Group: Z Natkaniec et al, Nucl. Instrum. Methods A 560, 1 (2006)Google Scholar
- [14]G C Fox and S Wolfram, Phys. Rev. Lett. 41, 1581 (1978)CrossRefADSGoogle Scholar
- [15]K A Olive et al, Chin. Phys. C 38, 090001 (2014)CrossRefADSGoogle Scholar
- [16]D J Lange, Nucl. Instrum. Methods A 462, 152 (2001)CrossRefADSGoogle Scholar
- [17]S Agostinelli et al, Nucl. Instrum. Methods A 506, 250 (2003)CrossRefADSGoogle Scholar
- [18]CLEO Collaboration: R Balest et al, Phys. Rev. D 52, 2661 (1995)Google Scholar
- [19]CLEO Collaboration: S Chen et al, Phys. Rev. D 63, 031102 (2001)Google Scholar
- [20]BABAR Collaboration: B Aubert et al, Phys. Rev. D 67, 032002 (2003)Google Scholar