Global Fit for D0-
  D0 Mixing
  
  (allowing for CP violation)
  
 (through 1 July 2021) 
   
 People working on this: 
 
 
Alan Schwartz,
Marco Gersabeck
For a complete list of references click 
 here 
For world average values of measured observables (used below) click 
 here 
 
 
 
 
 Notation: 
 
The mass eigenstates are denoted
D 1  ≡ p|D0> + 
q|D0> and
D 2  ≡ p|D0> − 
q|D0>;
δ and δKππ are strong phase differences
between 
D0
→ f  and D0 → f amplitudes, and 
φ is the weak phase difference Arg(q/p). We define
δ ≡
δ D0 → K−n(π) 
−
δ D0 
                   → K−n(π).
The mixing parameters are defined as 
x ≡ (m2 − m1)/Γ and
y ≡ (Γ2 − Γ1)/(2Γ), where
Γ = (Γ1 + Γ2)/2.
Our convention is (CP)|D0> = 
−|D0> 
and 
(CP)|D0> =
−|D0>; thus, in the absence of CP violation, 
x = (mCP+ − mCP−)/Γ and
y = (ΓCP+ − ΓCP−)/(2Γ).
 
 
 Experimental Observables: 
 
From all experiments there are 61 observables:
 
  y CP , 
  A Γ ,
  (x, y, |q/p|, φ) Belle  
   K0S π+ π − ,
  (xCP, yCP, Δx, Δy) LHCb  
   K0S π+ π − ,
  (x, y) BaBar
   K0S h+ h− ,
  (x, y) BaBar
   π0 π+ π− ,
  (R M )/2 LHCb  
   K+ π− π+ π − ,
  (R M ) semileptonic ,
  (x", y")
      K+ π− π 0 ,
  (R D , x2, y, cos δ, sin δ)
Ψ(3770) ,
  (RD, AD, x'2±, 
y'±)BaBar , 
  (RD, AD, x'2±, 
y'±)Belle , 
  (RD, x'2, y')CDF ,
  (RD±, x'2±, y'±)LHCb ,
(ACPK, 
ACPπ)BaBar ,
(ACPK, 
ACPπ)Belle ,
(ACPK − 
ACPπ)CDF ,
(ACPK −ACPπ)
LHCb(D*) ,
(ACPK −ACPπ)
LHCb(B →D0μX) 
 
 
 Theoretical Parameters: 
 
Allowing for CP violation, there are 10 underlying parameters:
 
  x, y, δ, δKππ, 
RD, 
AD, Aπ, AK, 
|q/p|, and Arg(q/p) = φ.
The first two parameters govern mixing; the next two are
strong phases; R D is the ratio 
Γ(D0→ 
f)/Γ(D0 → f);
the next three are direct CP-violating asymmetries for 
D0 → K+ π−, 
D0 → π+ π−, and
D0 → K+ K−, respectively;
and the last two are indirect CP-violating parameters.
The relationships between these parameters and the measured
observables are given below. The observables appear in 
 blue 
(on the left sides of the equations), the underlying parameters in 
  magenta 
(on the right sides), and intermediate variables in black.
  
 
 
   
Measurements used:  
  
  | Index | Observable | Value | Source | 
 
  | 1 | y CP | (0.719 ± 0.113)% | World average (COMBOS combination) 
   of D0 → K+ K− / 
    π+ π  −  /
    K+ K− K0 | 
 
  | 2 | A Γ | (0.0089 ± 0.0113)% | World average (COMBOS combination) 
   of D0 → K+ K− / 
    π+ π  −  results | 
|  |  
 | x (no CPV) |   | y (no CPV) |   |  |   |  |   | |q/p| (no dCPV) |   | Arg(q/p)=φ (no dCPV) |   |  |   |  |   | x |   | y |   | |q/p| |   | φ |  |  
 |  |   | 0.56 ± 0.19  +0.067   −0.127 |   | 0.30 ± 0.15  +0.050   −0.078 |   |  |   | 0.90  +0.16   −0.15 
 +0.078   −0.064 |   | (−6 ± 11  +4.2   −5 ) 
degrees |   |  |   | (0.58 ± 0.19  +0.0734   −0.1177 )% |   | (0.27 ± 0.16  +0.0546   −0.0854 )% |   | 0.82  +0.20   −0.18 
 +0.0807   −0.0645 |   | (−13  +12   −13 
 +4.15   −4.77 ) degrees |  | Belle    D0 → K0  S  
π+ π  −  results using
921 fb−1. 
 | Correlation coefficient is +0.012 for no-CPV; for CPV-allowed they are: |   
 
| 1 |  | 0.054 |  | −0.074 |  | −0.031 |   
| 0.054 |  | 1 |  | 0.034 |  | −0.019 |   
  
| −0.074 |  | 0.034 |  | 1 |  | 0.044 |   
  
| −0.031 |  | −0.019 |  | 0.044 |  | 1 |  | 
  |  |  
 | x (no CPV) |   | y (no CPV) |   |  |   | xCP |   | yCP |   | Δx |   | Δy |   |  |   | xCP |   | yCP |   | Δx |   | Δy |  |  
 | (−0.86 ± 0.53 ± 0.17)% |   | (0.03 ± 0.46 ± 0.13)% |   |  |   | (0.27 ± 0.16 ± 0.04)% |   | (0.74 ± 0.36 ± 0.11)% |   | (−0.053 ± 0.070 ± 0.022)% |   | (0.06 ± 0.16 ± 0.03)% |   |  |   | (0.397 ± 0.046 ± 0.029)% |   | (0.459 ± 0.120 ± 0.085)% |   | (−0.027 ± 0.018 ± 0.001)% |   | (0.020 ± 0.036 ± 0.013)% |  | 
 | LHCb  
   D0 → 
K0S π+π −  
results using 1 fb-1 (√s = 7 TeV) |   | D*+ → D0π+ flavor tag. 
Correlation coefficient = +0.37, no CPV. |   |  |   
| 3 fb-1 results  (√s = 7, 8 TeV) allowing for CPV. |   | D*+ → D0π+, 
B → D0μ− X flavor tags.
Correlation coefficients (stat. + syst.): |  
|  
 | 1 |  | (−0.17 + 0.15) |  | (0.04 + 0.01) |  | (−0.02 − 0.02) |   |  |  | 1 |  | (−0.03 − 0.05) |  | (0.01 − 0.03) |   |  |  |  |  | 1 |  | (−0.13 + 0.14) |  |   |  |   
| 5.4 fb-1 results  (√s = 13 TeV) allowing for CPV. |   | D*+ → D0π+ flavor tags.
Correlation coefficients (stat. + syst.): |  
|  
 | 1 |  | (0.11 + 0.13) |  | (−0.02 + 0.01) |  | (−0.01 + 0.01) |   |  |  | 1 |  | (−0.01 − 0.02) |  | (−0.05 + 0.01) |   |  |  |  |  | 1 |  | (0.08 + 0.31) |  |  
| For (x, y, |q/p|, φ) → (xCP, yCP, Δx, Δy) 
mapping, see 
 PRD 99, 012007 (2019) |  | 
  | 15-16 |  |  
 
| (0.16 ± 0.23 ± 0.12 ± 0.08)% |   
| (0.57 ± 0.20 ± 0.13 ± 0.07)% |  | 
 | BaBar  
   D0 → 
K0S π+π − and 
D0 → 
K0S K+ K − combined; |   | Correlation coefficient = +0.0615, no CPV. |  | 
 
  | 17-18 |  |  
 
| (1.5 ± 1.2 ± 0.6)% |   
| (0.2 ± 0.9 ± 0.5)% |  | 
 | BaBar  
   D0 → 
π0 π+π − |   | Correlation coefficient = −0.006, no CPV. |  | 
 
 
  | 19 | (x2 + y2)/2 | (0.0130 ± 0.0269)% | World average (COMBOS combination) 
   of 
D0 → K+l− ν results | 
 
  | 20-21 |  |  
 
| (2.61 +0.57 −0.68  ± 0.39)% |   
| (−0.06 +0.55 −0.64  ± 0.34)% |  | 
 | BaBar  
   K+ π  − π  0  result;
correlation coefficient = −0.75. |   | Note: x" = x cos δKππ + y sin δKππ,   
     y" = y cos δKππ − x sin δKππ. |  | 
 
  | 22-26 |  |  
 | (0.533 ± 0.107 ± 0.045)% |   | (0.06 ± 0.23 ± 0.11)% |   | (4.2 ± 2.0 ± 1.0)% |   | 0.81  +0.22−0.18
                           +0.07−0.05 |   | −0.01 ± 0.41 ± 0.04 |  | CLEO-c    Ψ(3770) results; correlation coefficients:  
 
| 1 |  | 0 |  | 0 |  | −0.42 |  | 0.01 |   
  
|  |  | 1 |  | −0.73 |  | 0.39 |  | 0.02 |  |   
  
|  |  |  |  | 1 |  | −0.53 |  | −0.03 |   
  
|  |  |  |  |  |  | 1 |  | 0.04 |   
|  |  |  |  |  |  |  |  | 1 |  | 
  | 27-29 |  |   
| (0.303 ± 0.0189)% |   
| (−0.024 ± 0.052)% |   
| (0.98 ± 0.78)% |  | BaBar   
  K+ π  − results; correlation coefficients:  
 
| 1 |  | +0.77 |  | −0.87 |   
| +0.77 |  | 1 |  | −0.94 |   
| −0.87 |  | −0.94 |  | 1 |  | 
 
  | 30-32 |  |   
| (−2.1 ± 5.4)% |   
| (−0.020 ± 0.050)% |   
| (0.96 ± 0.75)% |  | BaBar   
  K+ π  − results; correlation coefficients 
same as above. | 
  |  |  |   
| (0.353 ± 0.013)% |   
| (0.009 ± 0.022)% |   
| (0.46 ± 0.34)% |  | Belle  
 
  K+ π  − no-CPV results using 976 fb−1.
Correlation coefficients:   
| 1 |  | +0.737 |  | −0.865 |   
| +0.737 |  | 1 |  | −0.948 |   
| −0.865 |  | −0.948 |  | 1 |  | 
  | 33-35 |  |   
| (0.364 ± 0.018)% |   
| (0.032 ± 0.037)% |   
| (−0.12 ± 0.58)% |  | Belle   
  K+ π  − CPV-allowed results using 
400 fb−1. Correlation coefficients:   
| 1 |  | +0.655 |  | −0.834 |   
| +0.655 |  | 1 |  | −0.909 |   
| −0.834 |  | −0.909 |  | 1 |  | 
  | 36-38 |  |   
| (2.3 ± 4.7)% |   
| (0.006 ± 0.034)% |   
| (0.20 ± 0.54)% |  |  
 | Belle   
  K+ π  − CPV-allowed results using 
400 fb−1; |   | correlation coefficients same as above. |  | 
  | 39-41 |  |   
| (0.351 ± 0.035)% |   
| (0.008 ± 0.018)% |   
| (0.43 ± 0.43)% |  | CDF   
  K+ π  − results for 9.6 fb−1. 
Correlation coefficients:   
| 1 |  | 0.90 |  | −0.97 |   
| 0.90 |  | 1 |  | −0.98 |   
| −0.97 |  | −0.98 |  | 1 |  | 
  | 42-44 |  |   
| (0.338 ± 0.0161)% |   
| (−0.0019 ± 0.0447)% |   
| (0.581 ± 0.526)% |  | LHCb    K+ π  − results for 
3.0 fb−1  (√s = 7, 8 TeV) B → D*+μ− X, D*+ → D0π+  
flavor tags. Correlation coefficients:
   
| 1 |  | 0.823 |  | −0.920 |   
| 0.823 |  | 1 |  | −0.962 |   
| −0.920 |  | −0.962 |  | 1 |  | 
  | 45-47 |  |   
| (0.360 ± 0.0166)% |   
| (0.0079 ± 0.0433)% |   
| (0.332 ± 0.523)% |  | LHCb    K+ π  − results for 
3.0 fb−1  (√s = 7, 8 TeV) B → D*+μ− X, D*+ → D0π+ 
flavor tags. Correlation coefficients:
   
| 1 |  | 0.812 |  | −0.918 |   
| 0.812 |  | 1 |  | −0.956 |   
| −0.918 |  | −0.956 |  | 1 |  | 
  | 48-50 |  |   
| (0.3454 ± 0.0045)% |   
| (0.0061 ± 0.0037)% |   
| (0.501 ± 0.074)% |  | LHCb    K+ π  − results for 
5.0 fb−1  (√s = 7, 8 TeV) D*+ → D0π+ 
flavor tag. Correlation coefficients:
   
| 1 |  | 0.843 |  | −0.935 |   
| 0.843 |  | 1 |  | −0.963 |   
| −0.935 |  | −0.963 |  | 1 |  | 
  | 51-53 |  |   
| (0.3454 ± 0.0045)% |   
| (0.0016 ± 0.0039)% |   
| (0.554 ± 0.074)% |  | LHCb    K+ π  − results for 
5.0 fb−1  (√s = 7, 8 TeV) D*+ → D0π+ 
flavor tag. Correlation coefficients:
   
| 1 |  | 0.846 |  | −0.935 |   
| 0.846 |  | 1 |  | −0.964 |   
| −0.935 |  | −0.964 |  | 1 |  | 
  | 54-55 |  |  
 | (0.00 ± 0.34 ± 0.13)% |   | (−0.24 ± 0.52 ± 0.22)% |  | BaBar    385.8 fb−1 near ϒ(4S) resonance | 
  | 56-57 |  |  
 | (−0.43 ± 0.30 ± 0.11)% |   | (0.43 ± 0.52 ± 0.12)% |  | Belle    540 fb−1 near ϒ(4S) resonance | 
  | 58-59 |  |  
 | (−0.32 ± 0.21)% |   | (0.31 ± 0.22)% |  |  
 
| CDF    9.7 fb−1 
pp collisions at 
√s = 1.96 TeV |   | ( 〈t〉K − 〈t〉π )
/ τD = 0.27 ± 0.01 |  | 
  | 60 | ACPK − ACPπ | (−0.154 ± 0.029)% |  
 
| LHCb    8.9 fb−1 pp collisions at 
√s = 7, 8, 13 TeV |   
| D*+ → D0π+ 
and
B → D0μ− X flavor tags |   | ( 〈t〉K − 〈t〉π )/τD 
= 0.115 ± 0.002;  
〈t〉/τD 
= 1.71 ± 0.10 |  | 
  | 61 | (x2 + y2)/4 | (0.0048 ± 0.0018)% |  
 
| LHCb    3.0 fb−1 pp collisions at 
√s = 7, 8 TeV |   
| D0 → 
K+ π  − π  +  π  − |  | 
  
 MINUIT fit results 
  
  
 Five separate fits  are performed as follows:
 Fit #1:   
  
 no CP violation  
  
(AD= 0,   
AK= 0,    
Aπ= 0,    
|q/p| = 1,   φ = 0)
 Fits #2a and #2b:  
  
 no  direct  CP violation in doubly-Cabibbo-suppressed amplitudes   
  
(AD= 0)
In addition, we impose the relation  
tanφ = (1-|q/p|2)/(1+|q/p|2) × (x/y)
   
to reduce four independent parameters to three. This relation was first
derived by
Ciuchini et al. 
and was later independently obtained by 
Kagan and Sokoloff. 
Alternatively, one can use the quadratic equation (15) of
Grossman, Nir, and Perez  
to reduce four parameters to three
(e.g., see  here).
We use the Ciuchini/Kagan formula to perform two separate fits: first we 
float x, y, and φ and from them derive |q/p| (this yields proper errors 
for φ). Then we float x, y, and |q/p| and from them derive φ (this 
yields proper errors for |q/p|).
 Fit #2c:  
  
 no  direct  CP violation in doubly-Cabibbo-suppressed amplitudes   
  
(AD= 0)
fit for theory parameters x12, y12, and φ12
  
Here we fit for the underlying theory parameters
x12 ≡ 2|M12|/Γ,  
y12 ≡ |Γ12|/Γ,   
and φ12 ≡ Arg(M12/Γ12). 
The relationships between these parameters and our nominal 
parameters (x, y, |q/p|, φ) are given by
Kagan and Sokoloff   Eqs. (14, 15, 48, 52), but a 
factor of 2-1/2 is missing from Eqs. (14) and (15). 
An alternative derivation (our own) is  
 here;
these differ from Kagan and Sokoloff but give identical results.
 Fit #3:   
  
 allowing all CP violation  
  
(all parameters floated)
 The MINUIT output for all five fits (in order) are given
  here. 
(Note that x, y, R D, A D, A π and A K are in 
percent; δ, δ2 (=δKππ), and φ are in radians.)
  The final results are: 
 
 
Note that for the No-direct-CPV results, the values listed for 
(δ, δKππ, RD) are from Fit 2a
rather than Fit 2b (but they are almost identical).
   χ  2  contributions for CPV-allowed fit:  
 _____________________________________________
 
  _____________________________________________  
   
 MNCONTOUR-like 2-d plots: 
(click on for .eps versions)
   
 
 
           
 
 
   
 
CPV-allowed plot, no mixing (x,y) = (0,0) point:
  
Δ χ  2  = 2099,
  
excluded at ≫ 11.5σ (limit of CERNLIB PROB routine)
No CPV (|q/p|, φ) = (1,0) point:
  
Δ χ  2  = 5.633,
  
excluded at 1.56σ
 
   
 
 
 
           
   
 
 
 
           
 
 
   
 
  _____________________________________________  
 MNCONTOUR-like 1-d plots: 
Dashed  red 
horizontal line denotes Δχ  2 = 3.84, corresponding to
a 95% C.L. interval.
(click on for .eps versions) 
   
 
 
           
 
 
                        
x = 0 point:
  
Δ χ  2  = 68.30, 
  
x ≤ 0 excluded at 8.18σ
                
        
y = 0 point:
  
Δ χ  2  = 477.2, 
  
y ≤ 0 
excluded at > 11.4σ (limit of CERNLIB PROB)
 
   
 
 
 
           
 
 
   
 
 
 
           
 
 
  _____________________________________________  
   
 Comparison with results before LHCb's 5.4 fb−1 
D0 → 
K0S π+π −  
measurement, using identical binning: 
Left-most plots include all results 
 
except for
 
LHCb's 5.4 fb−1 D0 → 
K0S π+π −  
measurement of (xCP, yCP, Δx, Δy); 
right-most plots include that result too (all results).
(click on for .eps versions) 
   
 
 
           
 
 
   
 
 
 
           
 
 
   
   
This page is maintained by 
A. Schwartz
and was last updated