(EPSHEP 2015 conference)
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The results of the global CKM analysis include:

Numerical Results 
The global CKM fit in the (V_{ub},V_{cb}) plane:
Constraints in the (V_{ub},V_{cb}) plane.
The horizontal and vertical coloured bands represent our average of the determinations from semileptonic B decays.
The white bands with solid (dashed) borders correspond to the determination
from exclusive (inclusive) semileptonic B decays.
The diagonal coloured band corresponds to the determination of
V_{ub}/V_{cb} from Λ_{b} decays.
Our inputs and averages for V_{ub} are described in section 2.5 of the summary of inputs and results. The rainbow oval region indicates the indirect determination of V_{ub} and V_{cb} from the global fit, without any information from semileptonic or leptonic decays of bhadrons. 

Constraints on V_{ub} from inclusive and exclusive B decays, as well as our average, compared to the indirect determination from the global fit.  
Constraints on V_{cb} from inclusive and exclusive B decays, as well as our average, compared to the indirect determination from the global fit. 
Constraints on the angle α/ϕ_{2} from charmless B decays:
Constraints on α/ϕ_{2} from B→ππ, ρπ and ρρ (WA)



Constraints on α/ϕ_{2} from the combination of B→ππ, ρπ, and ρρ for BaBar, Belle and WA,
compared to the prediction from the global CKM fit (not including the αrelated measurements). 


Isospin triangles in B→ππ and B→ππ. One notices that the first triangle is flat, contrary to the second. 


Isospin triangles in B→ρρ and B→ρρ. Both triangles are flat. 

Pulls for various inputs or parameters involved in the Standard Model global fit.
Each pull (in units of σ) is computed by taking the square root of the difference between
χ^{2}_{min} obtained including or not including direct information on the quantity. This corresponds to consider
Δχ^{2}_{X;min}=χ^{2}_{with data on X;min}
χ^{2}_{without data X;min} as a random variable distributed with
1 degree of freedom, and reinterpret the probability of reaching the observed value in units of σ. The presence of a plateau in the Rfit model for theoretical uncertainties may lead to a vanishing pull for some quantities even in cases where the predicted and observed values are not identical. Many of the pulls presented in this plot are correlated [this is for instance the case for sin 2β and Br(B→τν)], so that the distribution of the corresponding pvalues should not be expected to be flat 
The global CKM fit in the large (ρ̅, η̅) plane:
Constraints in the (ρ̅, η̅) plane. The red hashed region of the global combination corresponds to 68% CL. 


Constraints in the (ρ̅, η̅) plane. The V_{ub} constraint has been splitted in three contributions: V_{ub} from inclusive and exclusive semileptonic B decays (plain dark green), V_{ub} from B^{+}→τ^{+} ν (hashed darker green), and V_{ub}/V_{cb} from Λ_{b} decays (hashed lighter green). The red hashed region of the global combination corresponds to 68% CL. 


Constraints in the (ρ̅, η̅) plane using only exclusive determinations of V_{ub} and V_{cb} from semileptonic decays as inputs. 


Constraints in the (ρ̅, η̅) plane using only inclusive determinations of V_{ub} and V_{cb} from semileptonic decays as inputs. 

The global CKM fit in the small (ρ̅, η̅) plane (zoom):
Zoomed constraints in the (ρ̅, η̅) plane.The red hashed region of the global combination corresponds to 68% CL. 


Zoomed constraints in the (ρ̅, η̅) plane. The V_{ub} constr aint has been splitted in three contributions: V_{ub} from inclusive and exclusive semileptonic B decays (plain dark green), V_{ub} from B^{+}→τ^{+} ν (hashed darker green), and V_{ub}/V_{cb} from Λ_{b} decays (hashed lighter green). The red hashed region of the global combination corresponds to 68% CL. 


Zoomed constraints in the (ρ̅, η̅) plane not including the angle measurements in the global fit. 


Constraints in the (ρ̅, η̅) plane including only the angle measurements. 


Constraints from CP conserving quantities (V_{ub} / V_{cb}, Δm_{d}, (Δm_{d} and Δm_{s}) and B^{+} →τ^{+} ν) in the (ρ̅, η̅) plane. 


Constraints from CP violating quantities (sin(2β), α, γ and ε_{k}) in the (ρ̅, η̅) plane. 


Constraints from "Tree" quantities in the (ρ̅, η̅) plane (involving γ(DK) and α from the isospin analysis with the help of sin2β (charmonium), which gives another tree only γ measurement (the only assumption is that the ΔI=3/2 b>d EW penguin amplitude is negligible)). 


Constraints from "Tree" quantities in the (ρ̅, η̅) plane (only γ(DK) is used). 


Constraints from "Tree" quantities in the (ρ̅, η̅) plane with only input on V_{ub} from semileptonic decays (ony γ(DK) is used). 


Constraints from "Tree" quantities in the (ρ̅, η̅) plane with only input on V_{ub} from exclusive semileptonic B decays (only γ(DK) is used). 


Constraints from "Tree" quantities in the (ρ̅, η̅) plane with only input on V_{ub} from inclusive semileptonic B decays (only γ(DK) is used). 


Constraints from "Loop" quantities in the (ρ̅, η̅) plane. 


Constraints in the (ρ̅, η̅) plane, not including the braching ratio of B^{+} → τ^{+}ν in the global fit. 


Constraints in the (ρ̅, η̅) plane not including the measurement of sin2β in the global fit. 

The global CKM fit in the large (ρ̅_{M}, η̅_{M}) plane with M = sb, ds, ct, ut, uc:
Constraints in the (ρ̅_{sb}, η̅_{sb}) plane. The red hashed region of the global combination corresponds to 68% CL. 


Constraints in the (ρ̅_{ds}, η̅_{ds}) plane. The red hashed region of the global combination corresponds to 68% CL. 


Constraints in the (ρ̅_{tc}, η̅_{tc}) plane. The red hashed region of the global combination corresponds to 68% CL. 


Constraints in the (ρ̅_{tu}, η̅_{tu}) plane. The red hashed region of the global combination corresponds to 68% CL. 


Constraints in the (ρ̅_{cu}, η̅_{cu}) plane. The red hashed region of the global combination corresponds to 68% CL. 

Constraint from the B^{+}→τ^{+} ν branching ratio:
There is a specific correlation between sin2β and BR(B→τν), regarding the prediction from the global fit without using these measurements. The cross corresponds to the experimental value with 1 sigma errors.  
The constraint can also be seen from the point of view of lattice inputs, with the predictions on the decay constant f_{Bd} and f_{Bd} Sqrt[B_{Bd}] 
Branching ratio of B_{s}→μ^{+} μ^{}
Prediction for Br(B_{s}→μ^{+} μ^{}), to be compared with the current measurement.  
Prediction on the two dileptonic branching ratios Br(B_{s}→μ^{+} μ^{}) and Br(B_{d}→μ^{+} μ^{}) coming from the global fit (without input on dileptonic branching ratios) compared to current experimental information. 
The global CKM fit in the (V_{ud},V_{us}) plane:
Constraints in the (V_{ud},V_{us}) plane. The indirect constraints (coming from b transitions) are related to V_{ud} and V_{us} through unitarity. The red hashed region of the global combination corresponds to 68% CL. 
The global CKM fit in the (V_{cd},V_{cs}) plane:
Constraints in the (V_{cd},V_{cs}) plane. The indirect constraints (combing from b and s transitions) are related to V_{cd} and V_{cs} through unitarity. The direct constraints combine leptonic and semileptonic D and D_{s} decays as well as information from neutrinonucleaon scattering and W → cs decays. The red hashed region of the global combination corresponds to 68% CL.  
Constraints in the (V_{cd},V_{cs}) plane where direct constraints involve only leptonic D and D_{s} decays with our inputs for lattice averages.  
Constraints in the (V_{cd},V_{cs}) plane where direct constraints involve only semileptonic D and D_{s} decays with our inputs for lattice averages.  
Constraints in the (V_{cd},V_{cs}) plane where direct constraints involve only information from neutrinonucleaon scattering and W→ cs decays (no lattice input). 
Constraints on the angle γ/ϕ_{3} from B decays to charm:
No update  See Summer 14 results (here). 
No update  See Summer 14 results (here). 
New physics in neutralmeson mixing:
No update  See Summer 14 results (here). 