Effects of Anomalous Tensor Couplings in Bs0−Bs0 Mixing
CHANG Qin1,2**, HAN Lin1, YANG Ya-Dong1,3
1Institute of Particle Physics, Huazhong Normal University, Wuhan 430079 2Department of Physics, Henan Normal University, Xinxiang, Henan 453007 3Key Laboratory of Quark & Lepton Physics (Ministry of Education), Huazhong Normal University, Wuhan 430079
Effects of Anomalous Tensor Couplings in Bs0−Bs0 Mixing
CHANG Qin1,2**, HAN Lin1, YANG Ya-Dong1,3
1Institute of Particle Physics, Huazhong Normal University, Wuhan 430079 2Department of Physics, Henan Normal University, Xinxiang, Henan 453007 3Key Laboratory of Quark & Lepton Physics (Ministry of Education), Huazhong Normal University, Wuhan 430079
摘要Motivated by the recently observed anomalous large dimuon charge asymmetry in neutral B decays, we study the effects of the anomalous tensor couplings to pursue a possible solution. With the constraints from the observables φsJ/ψ(φ,f0), asls and ΔMs, the new physics parameter spaces are severely restricted. We find that the contributions induced by the color−singlet or the color-octet tensor operators are helpful to moderate the anomaly in Bs0-Bs0 mixing. Numerically, the observable asls could be enhanced by about two orders of magnitude by the contributions of color−singlet or color-octet tensor operators with their respective nontrivial new weak phase φT1=41°±35° or φT8=−47°±33° and relevant strength parameters |gT1|=(2.89±1.40)×10−2 or |gT8|=(0.79±0.34)×10−2. However, due to the fact that the NP contributions are severely suppressed by the recent LHCb measurement for φsJ/ψ(φ,f0), our theoretical result of asls is still much smaller than the central value of the experimental data.
Abstract:Motivated by the recently observed anomalous large dimuon charge asymmetry in neutral B decays, we study the effects of the anomalous tensor couplings to pursue a possible solution. With the constraints from the observables φsJ/ψ(φ,f0), asls and ΔMs, the new physics parameter spaces are severely restricted. We find that the contributions induced by the color−singlet or the color-octet tensor operators are helpful to moderate the anomaly in Bs0-Bs0 mixing. Numerically, the observable asls could be enhanced by about two orders of magnitude by the contributions of color−singlet or color-octet tensor operators with their respective nontrivial new weak phase φT1=41°±35° or φT8=−47°±33° and relevant strength parameters |gT1|=(2.89±1.40)×10−2 or |gT8|=(0.79±0.34)×10−2. However, due to the fact that the NP contributions are severely suppressed by the recent LHCb measurement for φsJ/ψ(φ,f0), our theoretical result of asls is still much smaller than the central value of the experimental data.
CHANG Qin1,2**, HAN Lin1, YANG Ya-Dong1,3. Effects of Anomalous Tensor Couplings in Bs0−Bs0 Mixing[J]. 中国物理快报, 2012, 29(3): 31302-031302.
CHANG Qin, HAN Lin, YANG Ya-Dong. Effects of Anomalous Tensor Couplings in Bs0−Bs0 Mixing. Chin. Phys. Lett., 2012, 29(3): 31302-031302.
[1] Lenz A and Nierste U 2007 J. High Energy Phys. 0706 072
Lenz A 2008 Nucl. Phys. Proc. Suppl. 177 81
[2] Abulencia T et al (CDF collaboration) 2006 Phys. Rev. Lett. 97 242003
[3] Barberio E et al (HFAG) 2010 arXiv:1010.1589[hep-ex] and online update at http://www.slac.stanford.edu/xorg/hfag
[4] Abazov V M et al (D0 collaboration) 2011 arXiv:1109.3166[hep-ex]
[5] LHCb collaboration LHCb-CONF-2011-056
[6] Abazov V M et al (D0 collaboration) 2010 Phys. Rev. Lett. 105 081801
Abazov V M et al (D0 collaboration) 2010 Phys. Rev. D 82 032001
[7] Abazov V M et al (D0 collaboration) 2011 Phys. Rev. D 84 052007
[8] For a recent review, see: Lenz A, Nierste U and Charles J et al (CKMfitter Group) 2011 Phys. Rev. D 83 036004
[9] Chang Q, Li X Q and Yang Y D 2007 J. High Energy Phys. 0706 038
[10] Kim C S and Yang Y D 2004 arXiv:hep-ph/0412364
[11] Das P K and Yang K C 2005 Phys. Rev. D 71 094002
[12] Baek S, Datta A, Hamel P, Hernandez O F and London D 2005 Phys. Rev. D 72 094008
Baek S and London D 2007 Phys. Lett. B 653 249
Nandi S and Kundu A 2006 J. Phys. G 32 835
Alok A K, Dighe A and Sankar S U 2008 Phys. Rev. D 78 114025
Hatanaka H and Yang K C 2008 Phys. Rev. D 77 035013
Chang Q, Li X Q and Yang Y D 2008 J. High Energy Phys. 0809 038
[13] Buras A J, Jager S and Urban J 2001 Nucl. Phys. B 605 600
Buras A J, Misiak M and Urban J 2000 Nucl. Phys. B 586 397
[14] Buchalla G, Buras A J and Lautenbacher M E 1996 Rev. Mod. Phys. 68 1125
[15] Beneke M, Buchalla G and Dunietz I 1996 Phys. Rev. D 54 4419
Beneke M, Buchalla G, Lenz A and Nierste U 2003 Phys. Lett. B 576 173
[16] Nakamura K et al (Particle Data Group) 2010 J. Phys. G 37 075021
[17] Tevatron Electroweak Working Group, CDF collaboration and D0 collaboration 2008 arXiv:0808.1089[hep-ex]
[18] Bona M et al (UTfit collaboration) 2009 PMC Phys. A 3 6
[19] Gamiz E et al (HPQCD collaboration ) 2009 Phys. Rev. D 80 014503
[20] Becirevic D, Gimenez V, Martinelli G, Papinutto M and Reyes J 2002 J. High Energy Phys. 0204 025