A brief document that provides the collection of up-to-date inputs
to the global CKM analysis and the numerical results obtained from it.
The results include: Wolfenstein parameters, UT angles,
(combinations of) CKM elements, theory parameters and rare
branching fractions.
Detailed background information on the methodology and
the treatment of experimental and theoretical uncertainties
is provided in hep-ph/0406184.
Constraints in the (ρ-bar,η-bar) plane
with FPCP06 inputs and experimental measurements except
ΔMs as of Moriond 2006 (with D0 result but not CDF result).
Constraint in the (ρ-bar,η-bar) plane from the simultaneous
use of the the B+→τ+ν branching
fraction and Δmd with improved staggered fermions (see hep-lat/0510113).
Constraint in the (ρ-bar,η-bar) plane from the simultaneous
use of the limit on the B+→τ+ν branching
fraction and Δmd.
Also shown is the constraint one would obtain by a precise
measurement of BR(B+→τ+ν).
It illustrates the gain in accuracy obtained from the simultaneous use of the
two constraints ( B+→τ+ν and Δmd),
where the uncertainty from fB is reduced (it cancels in the ratio).
Constraints on α/Φ2 from B→ππ, ρπ, ρρ,
compared to the prediction from the CKM fit (not including these measurements).
α[combined] = 100.2 +15.0/–8.8 deg.
Constraints on γ/Φ3 from world average D(*)K decays
(GLW+ADS) and Dalitz analyses compared to the prediction from the global
CKM fit (not including these measurements).
γ[combined] = 62 +35/–25 deg.
Constraints on |sin(2β+γ)| from the measurement of time-dependent CP asymmetries in
D(*) π (ρ). Moriond06 HFAG average is used as input. The extraction of the UT angles relies on SU(3)
symmetry for the estimates of the suppressed-to-leading amplitude ratios. We use r = 0.013 ± 0.0023 and
r* = 0.019 ± 0.0029, and apply an additional theoretical uncertainty in form of a
15% error range to these.
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)|] = 71 +22 / – 30°