(EPS-HEP 2015 conference)
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The results of the global CKM analysis include:
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Numerical Results |
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.
Our inputs and averages for |Vub| are described in section 2.5 of the summary of inputs and results. 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. | |
Constraints on |Vcb| 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/ϕ2 from charmless B decays:
Constraints on α/ϕ2 from B→ππ, ρπ and ρρ (WA)
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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). |
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Isospin triangles in B→ππ and B→ππ. One notices that the first triangle is flat, contrary to the second. |
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Isospin triangles in B→ρρ and B→ρρ. Both triangles are flat. |
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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;min=χ2with 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 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 p-values 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. |
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Constraints in the (ρ̅, η̅) plane. The |Vub| constraint has been splitted 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 lighter green). The red hashed region of the global combination corresponds to 68% CL. |
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Constraints in the (ρ̅, η̅) plane using only exclusive determinations of |Vub| and |Vcb| from semileptonic decays as inputs. |
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Constraints in the (ρ̅, η̅) plane using only inclusive determinations of |Vub| and |Vcb| from semileptonic decays as inputs. |
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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. |
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Zoomed constraints in the (ρ̅, η̅) plane. The |Vub| constr aint has been splitted 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 lighter green). The red hashed region of the global combination corresponds to 68% CL. |
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Zoomed constraints in the (ρ̅, η̅) plane not including the angle measurements in the global fit. |
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Constraints in the (ρ̅, η̅) plane including only the angle measurements. |
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Constraints from CP conserving quantities (|Vub / Vcb|, Δmd, (Δmd and Δms) and B+ →τ+ ν) in the (ρ̅, η̅) plane. |
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Constraints from CP violating quantities (sin(2β), α, γ and εk) in the (ρ̅, η̅) plane. |
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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)). |
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Constraints from "Tree" quantities in the (ρ̅, η̅) plane (only γ(DK) is used). |
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Constraints from "Tree" quantities in the (ρ̅, η̅) plane with only input on |Vub| from semileptonic decays (ony γ(DK) is used). |
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Constraints from "Tree" quantities in the (ρ̅, η̅) plane with only input on |Vub| from exclusive semileptonic B decays (only γ(DK) is used). |
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Constraints from "Tree" quantities in the (ρ̅, η̅) plane with only input on |Vub| from inclusive semileptonic B decays (only γ(DK) is used). |
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Constraints from "Loop" quantities in the (ρ̅, η̅) plane. |
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Constraints in the (ρ̅, η̅) plane, not including the braching ratio of B+ → τ+ν in the global fit. |
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Constraints in the (ρ̅, η̅) plane not including the measurement of sin2β in the global fit. |
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The global CKM fit in the large (ρ̅M, η̅M) plane with
M = sb, ds, ct, ut, uc:
Constraints in the (ρ̅sb, η̅sb) plane. The red hashed region of the global combination corresponds to 68% CL. |
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Constraints in the (ρ̅ds, η̅ds) plane. The red hashed region of the global combination corresponds to 68% CL. |
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Constraints in the (ρ̅tc, η̅tc) plane. The red hashed region of the global combination corresponds to 68% CL. |
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Constraints in the (ρ̅tu, η̅tu) plane. The red hashed region of the global combination corresponds to 68% CL. |
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Constraints in the (ρ̅cu, η̅cu) plane. The red hashed region of the global combination corresponds to 68% CL. |
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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 fBd and fBd Sqrt[BBd] |
Prediction for Br(Bs→μ+ μ-), to be compared with the current measurement. | |
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. |
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. The red hashed region of the global combination corresponds to 68% CL. |
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-nucleaon scattering and W → cs decays. The red hashed region of the global combination corresponds to 68% CL. | |
Constraints in the (|Vcd|,|Vcs|) plane where direct constraints involve only leptonic D and Ds decays with our inputs for lattice averages. | |
Constraints in the (|Vcd|,|Vcs|) plane where direct constraints involve only semileptonic D and Ds decays with our inputs for lattice averages. | |
Constraints in the (|Vcd|,|Vcs|) plane where direct constraints involve only information from neutrino-nucleaon scattering and W→ cs decays (no lattice input). |
Constraints on the angle γ/ϕ3
from B decays to charm:
No update | See Summer 14 results (here). |
No update | See Summer 14 results (here). |
New physics in neutral-meson mixing:
No update | See Summer 14 results (here). |