Reconciling anomalous measurements in $B_s-{\bar{B}}_s$ mixing: the role of CPT-conserving and CPT-violating new physics

Abstract

Recently observed anomalies in the $B_s\to J/\ddot{I}ˆ\ddot{I}•$ decay and the like-sign dimuon asymmetry $A_{sl}^b$ hint at possible new physics (NP) in the $\bsbsbar$ mixing. We parameterize the NP with four model-independent quantities: the magnitudes and phases of the dispersive part $M_{12}$ and the absorptive part $\hat{I}{“}_{12}$ of the NP contribution to the effective Hamiltonian. We constrain these parameters using the four observables $\hat{I}”M_s$, $\hat{I}”\hat{I}{“}_s$, the mixing phase $β_s^{J/ψϕ}$, and $A_{sl}^b$. Our quantitative fit indicates that the NP should contribute a significant dispersive as well as absorptive part. In fact, models that do not contribute a new absorptive part are disfavored at more than 99% confidence level. We extend this formalism to include CPT violation, and show that CPT violation by itself, or even in presence of CPT-conserving new physics without an absorptive part, helps only marginally in the simultaneous resolution of these anomalies. The NP absorptive contribution to $\bsbsbar$ mixing therefore seems to be essential, and would imply a large branching fraction for channels like $B_s\to \ddot{I}{„}^{+}\ddot{I}{„}^{-}$.

The final version to be published in PRD. Earlier results updated (strengthened) with 9.1 fb^{-1} data from D0