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Numerical results:
The results of the global CKM analysis include:

Numerical Results 
The global CKM fit in the large (ρbar,ηbar) plane:
Constraints in the (ρbar,ηbar) plane. The Vub constraint has been splitted in the two contributions: Vub from inclusive and exclusive semileptonic decays (plain dark green) and Vub from B^{+}→τ^{+} ν (hashed green). The red hashed region of the global combination corresponds to 68% CL. 


Constraints in the (ρbar,ηbar) plane. The red hashed region of the global combination corresponds to 68% CL. 

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


Zoomed constraints in the (ρbar,ηbar) plane not including the angle measurements in the global fit. 


Zoomed constraints in the (ρbar,ηbar) plane including only the angle measurements in the global fit. 


Zoomed constraints in the (ρbar,ηbar) plane including the CP conserving quantities in the global fit, i.e., V_{ub} (semileptonic and B^{+}→τ^{+} ν), Δm_{d}, Δm_{d} & Δm_{s}. 


Zoomed constraints in the (ρbar,ηbar) plane including the CP violating quantities in the global fit, i.e., sin(2β), α, γ and ε_{K}. 


Zoomed constraints from "Tree" quantities in the (ρbar,ηbar) plane (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)). 


Zoomed constraints from "Loop" quantities in the (ρbar,ηbar) plane. 


Zoomed constraints in the (ρbar,ηbar) plane not including the braching ratio of B^{+} → τ^{+}ν in the global fit. 


Zoomed constraints in the (ρbar,ηbar) plane not including the measurement of sin2β in the global fit. 

The global CKM fit in the large ρ_{s}bar,η_{s}bar) plane:
Constraints in the (ρ_{s}bar,η_{s}bar) plane. The red hashed region of the global combination corresponds to 68% CL. 


Constraints on the angle β_{s} =arg(V_{ts}V_{tb}*/V_{cs}V_{cb}*) from the global CKM fit (no input from the timedependent CP asymmetry in B^{0}→J/ψφ decays is used.) 

Constraint from the B^{+}→τ^{+} ν branching ratio:
A new discrepancy in the CKM global fit has appeared, because of the new world average for sin2β, which is smaller than before, and the new world average for BR(B→τν). From the experimental point of view both new averages are in good agreement with previous determinations. 
There is a specific correlation between the two quantities in the global fit that is a bit at odds with the direct experimental determination. This is best viewed in the (sin2β,BR(B→τν)) plane, regarding the prediction from the global fit without using these measurements. The cross corresponds to the experimental values with 1 sigma uncertainties. 


The shape of the correlation can be understood by considering the ratio BR(B→τν)/Δm_{d}, where the decay constant f_{Bd} cancels, leaving limited theoretical uncertainties (the ratio depends only on the bag parameter B_{Bd}). Thus from the observables BR(B→τν) and Δm_{d} one gets an interesting constraint in the (ρbar,ηbar) plane, which does not match perfectly with the global fit output. 


To have a closer look, one can write the full formula for the ratio where one explicitly sees that the correlation between BR(B→τν) and the angle β is controlled by the values of B_{Bd}, and the angles α and γ. This can be checked explicitly by comparing the above analytical formula with the colored region in the (sin2β,BR(B→τν)) plane. In other words the discrepancy is not driven by the value of semileptonic V_{ub}, nor by the decay constant f_{Bd}. 

To quantify the discrepancy one can compare the indirect fit prediction for BR(B→τν) with the measurement. The deviation here is 2.4 sigmas. 


A simpler test is the comparison of the prediction of B_{Bd} from the above analytical formula (having only BR(B→τν), Δm_{d}, α, β, γ and V_{ud} as inputs, that is an almost completely theoryfree determination of B_{Bd}) with the current lattice determination B_{Bd} = 1.17 ^{+0.15}_{0.13}. For this test the deviation is 2.5 sigmas, dominated by the error on BR(B→τν), α, γ and B_{Bd}. 

Constraint from decays B →V γ:
Constraints on V_{td}/V_{ts} from exclusive b → d γ and b → s γ transitions, following the theoretical analysis of Ball et al. [hepph/0612081] and using the branching ratios of B → K^{*} γ (charged and neutral), ρ γ (charged and neutral), ω γ [our ICHEP08 average for the five channels], together with B_{s} → φ γ [0712.2659] and the asymmetry in B^{+} → ρ^{+} γ [0804.4770]. 


In the (ρbar, ηbar) plane, there is a large overlap with the constraints from B_{d} and B_{s} mixing, indicated with yellow and orange borders. 

Constraints on the angle α/ϕ_{2} from charmless B decays:
Constraint on α/ϕ_{2} from B→ππ compared to the prediction from the global CKM fit (not including the αrelated measurements). 


Constraint on α/ϕ_{2} from B→ρρ compared to the prediction from the global CKM fit (not including the αrelated measurements). 


Constraint on α/ϕ_{2} from B→ρπ (U and I only) compared to the prediction from the global CKM fit (not including the αrelated measurements). The global constraint on α from B→ρπ is a combination of the most recent BABAR and Belle data. This combination is not just a naive average in α but a combination in the 26 experimentally measured U and I coefficients which are correlated among each others. The correlation matrices are provided by both experiments (BABAR and Belle). The combined constraint has a preferred region around 120 degrees, and two suppressed regions around 30 and 85 degrees. 


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


Constraints from α in the (ρbar,ηbar) plane compared to the prediction from the global CKM fit (not including these αrelated measurements). 

Constraints on the angle γ/ϕ_{3} from B decays to charm:
Constraints on γ/ϕ_{3} from world average D(*)K(*) decays (GLW+ADS) and Dalitz analyses (GGSZ) compared to the prediction from the global CKM fit (not including these measurements): γ[combined] = (70^{+27}_{29})° 


Constraint on the ratio of interfering amplitudes r_{B} of the decay B → DK from world average D(*)K(*) decays (GLW+ADS) and Dalitz analyses (GGSZ): r_{B}(DK) = 0.087^{+0.022}_{0.018}. 


Constraint on the ratio of interfering amplitudes r_{B} of the decay B → DK from world average D(*)K(*) decays (GLW+ADS) and Dalitz analyses (GGSZ): r_{B}(DK) = 0.101 ^{+0.034}_{0.040}. 


Constraint on the ratio of amplitudes r_{B} of the decay B → DK^{*}: r_{B}(DK^{*})= 0.161^{+0.079}_{0.084}. 


Constraint on the strong phase between the interfering amplitudes of the decay B → DK from world average D(*)K(*) decays (GLW+ADS) and Dalitz analyses (GGSZ): δ_{B}(DK) = (110^{+22}_{27})°. 


Constraint on the strong phase between the interfering amplitudes of the decay B → D^{*}K: δ_{B}(D^{*}K) = (42^{+26}_{32})°. 


Constraint on the strong phase between the interfering amplitudes of the decay B → DK^{*}: δ_{B}(DK^{*}) = (47^{+103}_{28})°. 


Constraints from γ in the (ρbar,ηbar) plane compared to the prediction from the global CKM fit (not including these γrelated measurements). 

Constraints on sin(2β+γ):
Constraints on sin(2β+γ) from the measurement of timedependent CP asymmetries in D(*)π (ρ); Summer 08 HFAG average including a preliminary Belle ICHEP08 update for D*π is used as input. The extraction of the UTangle combination relies on SU(3) symmetry for the estimates of the suppressedtoleading amplitude ratios. We use for r^{(*)} the values of BABAR Collaboration, arXiv:0803.4296 [hepex] (aka Phys.Rev.D78:032005,2008) with an updated average for the ratio fDs/fD equal to 1.163 ± 0.007 (using recent inputs from ETMC08, FNALMILC07, and HPQCD07 Lattice groups) and treat the SU(3) uncertainty by using the method described in Max Baak's talk presented at CKM06 workshop (here) 


Translation of this result into γ (using sin(2β) as additional input and choosing among the four solutions to the SM one). γ[GLW+ADS+GGSZ+sin(2β+γ)] = (76 ^{+16}_{23})°. 


Constraints from sin(2β+γ) in the (ρbar,ηbar) plane. 

Constraints on New physics in B_{d,s}Meson Mixing:
individual constraints correspond to 68% CL (see: arXiv:1008.1593 [hepph]). 
Constraints on New Physics in the (ReΔ_{d},ImΔ_{d}) plane from B_{d}meson mixing. 


Constraints on New Physics in the (ReΔ_{s},ImΔ_{s}) plane from B_{s}meson mixing. 
