in the light of recent LHCb data
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Reference 
Scenario I 
Scenario II 
Scenario III 
Scenario IV 
Some of the plots below come from the following paper:
This update includes the results up to the end of 2011, including the CDF [arXiv:1112.1726] and LHCb [arXiv:1112.3183] results on (φ_{s},ΔΓ_{s}) from B_{s}>J/Ψ Φ. It corresponds to the first version of arXiv:1203.0238. 
In scenario I we have introduced NP in
M_{12}^{q} = M_{12}^{SM,q}Δ_{q} independently for B_{d}, B_{s} and K, corresponding to NP with arbitrary flavour structure.
Constraint for B_{d} mixing: 


Constraint for B_{s} mixing: and Im Δ_{s}=0.04^{+0.17}_{0.17}. 


Indirect constraint on the asymmetry A_{SL}=(15.5^{+14.3}_{5.9})10^{4} compared with the direct measurements of CDF and D0. 


Indirect constraint on the CP phase φ_{s}^{J/Ψ Φ}=123.9^{+9.0}_{13.6}ˆ or 61.8^{+13.4}_{8.9}ˆ compared with the direct measurements of CDF, D0 and LHCb. 

In scenario II we have introduced NP in M_{12}^{q} = M_{12}^{SM,q}Δ_{q} with Minimal Flavour Violation (MFV) with small bottom Yukawa coupling yielding Δ_{d}=Δ_{s}=Δ real. Constraint for neutral meson mixing Δ=0.895^{+.069}_{0.063}. 

In scenario III we have introduced NP in
M_{12}^{q} = M_{12}^{SM,q}Δ_{q} with Minimal Flavour Violation (MFV) with large bottom Yukawa coupling
yielding Δ_{d}=Δ_{s}=Δ complex.
Constraint for B_{d} and B_{s} mixings: 

In order to accomodate the measurements of φ_{s} and A_{SL}, we introduce a fourth scenario with NP occurring not only in M_{12}^{q}, but also Gamma;_{12}^{q}. We introduce the new parameters


Constraint for Im(δ_{d}) and Im(δ_{s}) with the 68% CL intervals Im(δ_{d})=0.92^{+1.11}_{0.69} and Im(δ_{s})=1.2^{+1.6}_{1.0}. The pvalue for the 2D SM hypothesis Im(δ_{d})= Im(δ_{d}^{SM}) and Im(δ_{s})= Im(δ_{s}^{SM}) is 3.2 σ. 


Constraint for Re(δ_{s}) and Im(δ_{s}). The pvalue for the SM hypothesis δ_{d,s}= δ_{d,s}^{SM} and Δ_{d}=Δ_{s}=1 is 2.8 σ. 
