Results as of EPS 2005
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A brief document that provides the collection of uptodate 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 hepph/0406184. 
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The global CKM fit in the large (ρbar,ηbar) plane:
α,β,γ convention:  φ_{1},φ_{2},φ_{3} convention:  
Constraints in the (ρbar,ηbar) plane including (a.o.) the most recent α/Φ_{2} and γ/Φ_{3}related inputs in the global CKM fit. 
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Constraints in the (ρbar,ηbar) plane not including the angle measurements in the global fit. 
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Constraints in the (ρbar,ηbar) plane not including the α/Φ_{2} and γ/Φ_{3} measurement in the global fit. the global fit. 
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Constraints in the (ρbar,ηbar) plane including only the angle measurements in the global fit. 
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"Movie" showing stepbystep the constraints in the (ρbar,ηbar) plane  PPT FILE 
The global CKM fit in the small (ρbar,ηbar) plane (zoom):
α,β,γ convention:  φ_{1},φ_{2},φ_{3} convention:  
Zoomed constraints in the (ρbar,ηbar) plane including the most recent α/Φ_{2} and γ/Φ_{3}related inputs in the global CKM fit. 
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Zoomed constraints in the (ρbar,ηbar) plane not including the angle measurements in the global fit. 
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Constraints in the (ρbar,ηbar) plane including only the angle measurements in the global fit. 
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Constraints on the angle α/Φ_{2} from charmless B decays:
Constraint on α/Φ_{2} from B→ππ. 
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Constraint on α/Φ_{2} from B→ρρ. 
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Constraints on α/Φ_{2} from B→ππ, ρπ, ρρ, compared to the prediction from the CKM fit (not including these measurements). α[combined] = 98.6 +12.6/–8.1 deg. 
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Constraint in the (ρbar,ηbar) plane from B→ππ, ρπ, ρρ, compared with the global CKM fit (not including these αrelated measurements). 
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The numerical results for these quantities are given in the summary paper.  
Constraints on the angle γ/Φ_{3} from B decays to charm (to be updated):
Constraints on γ/Φ_{3} 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] = 63 +15/–12 deg. 
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Constraints on γ/Φ_{3} from world average D(*)K decays (GLW+ADS) and Dalitz analyses from BABAR compared to the prediction from the global CKM fit (not including these measurements). 
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α,β,γ convention:  φ_{1},φ_{2},φ_{3} convention:  
Constraints in the (ρbar,ηbar) plane on γ/Φ_{3} from world average D(*)K decays (GLW+ADS) and Dalitz analyses compared to the prediction from the global CKM fit (not including these measurements). 
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Constraints in the (ρbar,ηbar) plane on γ/Φ_{3} from world average D(*)K decays (GLW+ADS) and Dalitz analyses from BABAR compared to the prediction from the global CKM fit (not including these measurements). 
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The numerical results for these quantities are given in the summary paper.  
Constraints on the angle β_{s} (= δγ):
Constraints on the angle β_{s} =arg(V_{ts}V_{tb}*/V_{cs}V_{cb}*) (upper plot) and sin(2β_{s}) (lower plot) from the global CKM fit (no direct measurement from the timedependent CP asymmetry in B^{0}→J/ψφ decays is available yet). 
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The numerical results for these quantities are given in the summary paper.  
Constraint from limit on the B^{+}→τ^{+} ν
branching fraction:
Constraint in the (ρbar,ηbar) plane from the simultaneous use of the limit on the B^{+}→τ^{+}ν branching fraction and Δm_{d}. 
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Constraint in the (ρbar,ηbar) plane from the simultaneous use of the limit on the B^{+}→τ^{+}ν branching fraction and Δm_{d}. Also shown is the constraint one would obtain by a precise measurement of BR(B+>tau+nu). It illustrates the gain in accuracy obtained from the simultaneous use of the two constraints ( B^{+}→τ^{+}ν and Δm_{d}), where the uncertainty from fB is reduced (it cancels in the ratio). 
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Constraint in the (ρbar,ηbar) plane from the branching fraction (B^{0}→ρ^{0} γ / B^{0}→K^{*0} γ). Average BABAR and Belle. 
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Constraint in the (ρbar,ηbar) plane (not including the angle measurements in the global fit) from the branching fraction (B^{0}→ρ^{0} γ / B^{0}→K^{*0} γ). Average BABAR and Belle. 
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Constraint in the (ρbar,ηbar) plane from the branching fraction (B^{0}→ρ^{0} γ / B^{0}→K^{*0} γ). BABAR only. 
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Constraint in the (ρbar,ηbar) plane from the ratio of the branching fractions (B→ργ / B→K^{*} γ) where the average of neutral and charged B decays (and average of BABAR and Belle) has been used. 
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Constraint in the (ρbar,ηbar) plane (not including the angle measurements in the global fit) from the ratio of the branching fractions (B→ργ / B→K^{*} γ) where the average of neutral and charged B decays (and average of BABAR and Belle) has been used. 
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Constraints on sin(2β+γ) from the measurement of timedependent CP asymmetries in D^{(*)} π (ρ). Moriond05 HFAG average is used as input. The extraction of the UT angles relies on SU(3) symmetry for the estimates of the suppressedtoleading amplitude ratios. We use r = 0.019 ± 0.004 and r^{*} = 0.015 + 0.004 / – 0.006 , and apply an additional theoretical uncertainty in form of a 30% error range to these. 
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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)] = 70 +12 / – 14° 
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Constraints from sin(2β+γ) in the (ρbar,ηbar) plane. 
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Constraints from CP conserving quantities (V_{ub} / V_{cb}, Δm_{d}, (Δm_{d} and Δm_{s}) and B^{+}→τ^{+} ν) in the (ρbar,ηbar) plane. 
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Constraints from CP violating quantities (sin(2β), α, γ and ε_{k}) in the (ρbar,ηbar) plane. 
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Constraints from V_{ub} / V_{cb} and s to d transition in the (ρbar,ηbar) plane. 
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Constraints from V_{ub} / V_{cb} and b to d transition in the (ρbar,ηbar) plane. 
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Constraints from V_{ub} / V_{cb} and b to s transition in the (ρbar,ηbar) plane. 
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New physics in B^{0} B^{0}bar Mixing :
New physics in B^{0} B^{0}bar Mixing can be described modelindependently by
introducing two new parameters measuring the relative strength (r_{d}^{2})
and the relative phase between the B^{0} B^{0}bar mixing matrix element
containing contributions from SM as well as from NP contributions
compared to SM contributions only:


Constraints from V_{cb} + V_{ub} , Δm_{d}=Δm_{d}^{{SM}} * r_{d}^{2} and sin(2β+2Θ_{d}) in the (ρbar,ηbar) plane. 
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Constraints from V_{cb} + V_{ub} , Δm_{d}=Δm_{d}^{{SM}} * r_{d}^{2} and sin(2β+2Θ_{d}) in the (2Θ_{d} , r_{d}^{2}) plane. 
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Since there are four free parameters in the fit (ρbar,ηbar,2*Θ_{d},r_{d}^{2})
but only three constraints depend on those there is no other constraint in the
(ρbar,ηbar) plane visible but the one coming from V_{ub} and V_{cb} alone.
As a consequence, the allowed region in the (2*Θ_{d},r_{d}^{2}) plane is large.
When using in addition the following inputs: cos(2β) > 0 (suggested by data), α (ππ, 3π, ρρ), γ the allowed regions are substantially reduced: 

in the (ρbar,ηbar) plane. 
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in the (2*Θ_{d},r_{d}^{2}) plane. 
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There are two solutions left. The SM solution (2*Θ_{d} = 0 ,r_{d}^{2} = 1) is prefered. If the other solution can be eliminated with more data the possible additional phase from NP could not be very large (<15 degree). The relative strength of NP to SM contributions can still easily be of order 100%. 