Preliminary results as of Summer 2016
(ICHEP 2016 conference)

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The global CKM fit: Inputs and Numerical results
The global CKM fit: Pulls
The global CKM fit in the large (ρ-bar,η-bar) plane
Constraint on Vub versus sin(2β)
Branching ratio of Bs→μ+ μ-
The global CKM fit in the small (ρ-bar,η-bar) plane (zoom)
The global CKM fit in the large (ρ̅M, η̅M) plane with M = sb, ds, ct, ut, uc
The global CKM fit in the (|Vud|,|Vus) plane
The global CKM fit in the (|Vcd|,|Vcs) plane
The global CKM fit in the (|Vub|,|Vcb) plane
Constraints on the angle α/ϕ2 from charmless B decays
Constraints on the angle γ/ϕ3 from B decays to charm


Numerical results:

The results of the global CKM analysis include:

  • Wolfenstein parameters,
  • UT angles and sides,
  • UTsangle and apex,
  • CKM elements,
  • theory parameters,
  • rare branching fractions (B->lν, B->ll).

Numerical Results

The global CKM fit in the large (ρ-bar,η-bar) plane:

Constraints in the (ρ-bar,η-bar) plane. The red hashed region of the global combination corresponds to 68% CL.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints in the (ρ-bar,η-bar) plane. The |Vub| constraint has been split in three contributions: |Vub| from inclusive and exclusive semileptonic B decays (plain dark green), |Vub| from B+→τ+ ν (hashed darker green), and |Vub|/|Vcb| from Λb decays (hashed ligher green). The red hashed region of the global combination corresponds to 68% CL.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints in the (ρ̅, η̅) plane using only exclusive determinations of |Vub| and |Vcb| from semileptonic B decays as inputs.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints in the (ρ̅, η̅) plane using only inclusive determinations of |Vub| and |Vcb| from semileptonic B decays as inputs.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraint on Vub versus sin(2β):

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.


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A similar correlation can be found between sin2β and |Vub|SL, regarding the prediction from the global fit without using these measurements. The cross corresponds to the experimental value with 1 sigma errors.


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Branching ratio of Bs→μ+ μ-

Prediction for Br(Bs→μ+ μ-)=(3.25+0.15-0.13)x10-9, to be compared with the current measurement (we consider here the branching ratio at t=0, not including effects due to Bs mixing).


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Prediction on the two dileptonic branching ratios Br(Bs→μ+ μ-) and Br(Bd→μ+ μ-) coming from the global fit (without input on dileptonic branching ratios) compared to current experimental information.


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The global CKM fit in the small (ρ-bar,η-bar) plane (zoom):

Zoomed constraints in the (ρ-bar,η-bar) plane.The red hashed region of the global combination corresponds to 68% CL.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Zoomed constraints in the (ρ-bar,η-bar) plane. The |Vub| constraint has been split in three contributions: |Vub| from inclusive and exclusive semileptonic B decays (plain dark green), |Vub| from B+→τ+ ν (hashed darker green), and |Vub|/|Vcb| from Λb decays (hashed ligher green). The red hashed region of the global combination corresponds to 68% CL.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Zoomed constraints in the (ρ-bar,η-bar) plane not including the angle measurements in the global fit.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints in the (ρ-bar,η-bar) plane including only the angle measurements.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints from CP conserving quantities (|Vub / Vcb|, Δmd, (Δmd and Δms) and B+ →τ+ ν) in the (ρ-bar,η-bar) plane.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints from CP violating quantities (sin(2β), α, γ and εk) in the (ρ-bar,η-bar) plane.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints from "Tree" quantities in the (ρ-bar,η-bar) 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)).
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints from "Tree" quantities in the (ρ-bar,η-bar) plane (only γ(DK) is used).
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints from "Tree" quantities in the (ρ-bar,η-bar) plane with only input on |Vub| from semileptonic decays (ony γ(DK) is used).
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints from "Tree" quantities in the (ρ-bar,η-bar) plane with only input on |Vub| from exclusive semileptonic B decays (only γ(DK) is used).
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints from "Tree" quantities in the (ρ-bar,η-bar) plane with only input on |Vub| from inclusive semileptonic B decays (only γ(DK) is used).
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints from "Loop" quantities in the (ρ-bar,η-bar) plane.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints in the (ρ-bar,η-bar) plane, not including the braching ratio of B+ → τ+ν in the global fit.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints in the (ρ-bar,η-bar) plane not including the measurement of sin2β in the global fit.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Pulls

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 χ2min obtained including or not including direct information on the quantity. This corresponds to consider Δχ2X;min2with data on X;min- χ2without 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 systematic uncertainties may lead to a vanishing pull for some quantities even in cases where the predicted and observed values are not identical. Some of the pulls presented in this plot are correlated [this is for instance the case for sin 2β and Br(B→τν)].


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The global CKM fit in the large (ρ̅M, η̅M) plane
with M = sb, ds, ct, ut, uc:

The constraints can be expressed in the unitarity triangles associated with the different mesons of interest, with the relative coordinates of the upper appex of each triangle defined as
ρ̅d1d2+iη̅d1d2 =-(Vud1Vud2*)/(Vcd1Vcd2*),     ρ̅u1u2+iη̅u1u2 =-(Vu1dVu2d*)/(Vu1sVu2s*).
Constraints in the (ρ̅sb, η̅sb) plane. The red hashed region of the global combination corresponds to 68% CL.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints in the (ρ̅ds, η̅ds) plane. The red hashed region of the global combination corresponds to 68% CL.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints in the (ρ̅tc, η̅tc) plane. The red hashed region of the global combination corresponds to 68% CL.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints in the (ρ̅tu, η̅tu) plane. The red hashed region of the global combination corresponds to 68% CL.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints in the (ρ̅cu, η̅cu) plane. The red hashed region of the global combination corresponds to 68% CL.
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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The global CKM fit in the (|Vud|,|Vus|) plane:

Constraints in the (|Vud|,|Vus|) plane. The indirect constraints (coming from b transitions) are related to |Vud| and |Vus| through unitarity. Kl3 decays exhibit a discrepancy compared to other measurements.


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Prediction for the normalisation of the vector form factor FK→π+(0), compared to our current average of lattice results, indicating a discrepancy between the two values.


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The global CKM fit in the (|Vcd|,|Vcs|) plane:

Constraints in the (|Vcd|,|Vcs|) plane. The indirect constraints (combing from b and s transitions) are related to |Vcd| and |Vcs| through unitarity. The direct constraints combine leptonic and semileptonic D and Ds decays as well as information from neutrino-nucleon scattering and W → cs decays. The red hashed region of the global combination corresponds to 68% CL.


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Constraints in the (|Vcd|,|Vcs|) plane where direct constraints involve only leptonic D and Ds decays.


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Constraints in the (|Vcd|,|Vcs|) plane where direct constraints involve only semileptonic D and Ds decays.


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Constraints in the (|Vcd|,|Vcs|) plane where direct constraints involve only information from neutrino-nucleaon scattering and W→ cs decays (no lattice input).


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The global CKM fit in the (|Vub|,|Vcb|) plane:

Constraints in the (|Vub|,|Vcb|) 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 |Vub|/|Vcb| from Λb decays.

The rainbow oval region indicates the indirect determination of |Vub| and |Vcb| from the global fit, without any information from semileptonic or leptonic decays of b-hadrons.


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Constraints on |Vub| from inclusive and exclusive B decays, as well as our average, compared to the indirect determination from the global fit.


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Constraints on |Vcb| from inclusive and exclusive B decays, as well as our average, compared to the indirect determination from the global fit.


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Constraints on the angle α/ϕ2 from charmless B decays:

Constraints on α/ϕ2 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 α-related measurements).
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints on α/ϕ2 from B→ππ, ρπ and ρρ (WA) compared to the prediction from the global CKM fit (not including the α-related measurements).
α, β, γ
convention
ϕ1, ϕ2, ϕ3
convention

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Constraints on the angle γ/ϕ3 from B decays to charm :

Constraints on γ/ϕ3 from all measurements on D(*)K(*) decays (GLW+ADS) and Dalitz analyses (GGSZ) (experiments shown separately): γ[combined] = 72.2+5.3-5.8°. The result includes all data from B-factores and LHCb Run I.


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