People working on this:
David Asner,
Bostjan Golob,
Alan Schwartz
For a complete list of references click
here
Notation:
the mass eigenstates are denoted
D 1 ≡ p|D0> +
q|D0> and
D 2 ≡ p|D0> −
q|D0>;
R D is the ratio of magnitudes of D0 → f
and
D0 → f
amplitudes;
δ and δKππ are strong phase differences
between
D0
→ f and D0 → f amplitudes, and
φ is a weak phase difference.
The mixing parameters are defined as
x ≡ (m2 − m1)/Γ and
y ≡ (Γ2 − Γ1)/(2Γ), where
Γ = (Γ1 + Γ2)/2.
In the absence of CP violation, our convention is
x = (mCP+ − mCP−)/Γ,
y = (ΓCP+ − ΓCP−)/(2Γ), and
δ =
δ D0
→ K+n(π)
−
δ D0 → K+n(π) .
The following "pure" measurements and their world averages are presented:
D0 → K+l− ν results for R M ≡ (x2+y2)/2.
Year | Experiment | Result | Comment | |||||
---|---|---|---|---|---|---|---|---|
1996 | FNAL E791 | R M = (0.11 +0.30 −0.27 +0.00 −0.014 )% | 500 GeV π −N interactions (2 × 1010 events) | |||||
2005 | CLEO II.V | R M = (0.16 ± 0.29 ± 0.29 )% | 9.0 fb−1 near Υ(4S) resonance | |||||
2004 | BaBar | R M = (0.23 ± 0.12 ± 0.04 )% | 87 fb−1 near Υ(4S) resonance | |||||
2007 | BaBar | R M = (0.004 +0.070 −0.060 )% |
|
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2008 | Belle | R M = (0.013 ± 0.022 ± 0.020 )% | 492 fb−1 near Υ(4S) resonance | |||||
COMBOS average |
|
|
D0 → K+ K−, π+ π−, K+ K− K0 results for: y CP ≡ [Γ(CP+)/<Γ>]−1 = (1/2)(|q/p| + |p/q|) y cosφ − (1/2)(|q/p| − |p/q|) x sin φ, and A Γ ≡ [τ(D0 → K+ K−) − τ(D0 → K+ K− )] / [τ(D0 → K+ K−) + τ(D0 → K+ K− )] = (1/2)(|q/p|−|p/q|) y cosφ −(1/2)(|q/p|+|p/q|) x sin φ .
Year | Experiment | Result | Comment | ||||||||
---|---|---|---|---|---|---|---|---|---|---|---|
1999 | FNAL E791 | ΔΓ = (0.04 ± 0.14 ± 0.05 ) ps −1 | 500 GeV π −N interactions (2 × 1010 events) | ||||||||
2000 | FOCUS | y CP = (3.42 ± 1.39 ± 0.74 )% | γN interactions (1 × 106 reconstr. D → K n(π) decays) | ||||||||
2002 | CLEO II.V | y CP = (−1.2 ± 2.5 ± 1.4 )% | 9.0 fb−1 near Υ(4S) resonance | ||||||||
2002 | Belle | y CP = (−0.5 ± 1.0 +0.7 −0.8 )% | 23.4 fb−1 near Υ(4S) resonance; no D* tag | ||||||||
2007 | Belle |
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540 fb−1 near Υ(4S) resonance | ||||||||
2008 | BaBar |
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2009 | BaBar |
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2009 | Belle |
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673 fb−1 near Υ(4S) resonance, D → (K+K−) K0 decays | ||||||||
COMBOS average |
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|
Plot of y CP average: Plot of A Γ average:
D0 → K+ π − results for: R D, x' ≡ x cosδ + y sin δ, y' ≡ y cosδ - x sin δ, and R B ≡ R D + y' √ R D + (x2+y2)/2 . These results assume no CPV; for results allowing for CPV click here
Year | Experiment | Result | Comment | ||||
---|---|---|---|---|---|---|---|
1998 | FNAL E791 | RB = (0.68 +0.34 −0.33 ± 0.07)% | 500 GeV π −N interactions (2 × 1010 events) | ||||
2000 | CLEO II.V |
|
9.0 fb−1 near Υ(4S) resonance | ||||
2005 | FOCUS |
|
γN interactions (1 × 106 reconstr. D → K n(π) decays) | ||||
2006 | Belle |
|
400 fb−1 near Υ(4S) resonance | ||||
2007 | BaBar |
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384 fb−1 near Υ(4S) resonance | ||||
2007 | CDF (Run II) |
|
1.5 fb−1 at √s = 1.96 TeV (Tevatron) |
D0 → K+ π − π 0 and K+ π − π + π − results for: R B, R M, <R D>, and α<y'>, where <…> denotes a quantity integrated (or averaged) over the selected phase-space region of the Dalitz plot, and α is a suppression factor in the range (0,1) arising from strong phase differences over the Dalitz plot. For D0 → K+ π − π 0 there is a strong phase difference δKππ (analogous to δ in D0 → K+ π − decays): x" ≡ x cosδKππ + y sin δKππ, y" ≡ y cosδKππ - x sin δKππ. These results assume no CPV.
Year | Experiment | Result | Comment | |||||
---|---|---|---|---|---|---|---|---|
2005 | Belle |
|
281 fb−1 near Υ(4S) resonance | |||||
2006 | BaBar |
|
230.4 fb−1 near Υ(4S) resonance | |||||
2006 | BaBar |
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230.4 fb−1 near Υ(4S) resonance | |||||
2008 | BaBar |
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384 fb−1 near Υ(4S) resonance |
D0 → K0S π+ π − results. These results assume no CPV; for results allowing for CPV click here
Year | Experiment | Result | Comment | |||||
---|---|---|---|---|---|---|---|---|
2005/2007 | CLEO II.V |
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2007 | Belle |
|
540 fb−1 near Υ(4S) resonance | |||||
COMBOS average |
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Ψ(3770) → D0-D0 results, using correlations. The upper measurements are obtained from a fit that uses externally measured branching fractions as input, but no externally measured mixing parameters; the lower measurement is obtained from a fit that uses (in addition to branching fractions) externally measured values of RM and RD.
Year | Experiment | Result | Comment | |||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|
2008 | CLEOc |
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0.281 fb−1 at Ψ(3770) resonance | ||||||||
cos δ | 1.10 ± 0.35 ± 0.07 |
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