CONSTRAINED FIT INFORMATION show precise values?
 
An overall fit to 68 branching ratios uses 134 measurements and one constraint to determine 34 parameters. The overall fit has a $\chi {}^{2}$ = 149.3 for 101 degrees of freedom.
 
The following off-diagonal array elements are the correlation coefficients <$\mathit \delta $x$_{i}$~$\delta $x$_{j}$> $/$ ($\mathit \delta $x$_{i}\cdot{}\delta $x$_{j}$), in percent, from the fit to parameters ${{\mathit p}_{{i}}}$, including the branching fractions, $\mathit x_{i}$ =$\Gamma _{i}$ $/$ $\Gamma _{total}$. The fit constrains the ${{\mathit x}_{{i}}}$ whose labels appear in this array to sum to one.
 
 x6  100
 x19   100
 x20    100
 x21     100
 x30      100
 x31       100
 x37        100
 x38         100
 x43          100
 x58           100
 x77            100
 x88             100
 x94              100
 x103               100
 x117                100
 x118                 100
 x119                  100
 x133                   100
 x140                    100
 x141                     100
 x142                      100
 x160                       100
 x189                        100
 x203                         100
 x205                          100
 x209                           100
 x210                            100
 x211                             100
 x212                              100
 x223                               100
 x284                                100
 x288                                 100
 x295                                  100
 x355                                   100
   x6  x19  x20  x21  x30  x31  x37  x38  x43  x58  x77  x88  x94  x103  x117  x118  x119  x133  x140  x141  x142  x160  x189  x203  x205  x209  x210  x211  x212  x223  x284  x288  x295  x355
 
  Mode Fraction (Γi / Γ)Scale factor

Γ6  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \mu}^{+}}$ anything $0.068$ $\pm0.006$ 
Γ19  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit e}^{+}}{{\mathit \nu}_{{e}}}$  $0.03549$ $\pm0.00026$ 1.2
Γ20  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \mu}^{+}}{{\mathit \nu}_{{\mu}}}$  $0.0341$ $\pm0.0004$ 1.0
Γ21  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{*}{(892)}^{-}}{{\mathit e}^{+}}{{\mathit \nu}_{{e}}}$  $0.0215$ $\pm0.0016$ 
Γ30  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \pi}^{-}}{{\mathit e}^{+}}{{\mathit \nu}_{{e}}}$  ($2.91$ $\pm0.04$) $ \times 10^{-3}$ 1.0
Γ31  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \pi}^{-}}{{\mathit \mu}^{+}}{{\mathit \nu}_{{\mu}}}$  ($2.67$ $\pm0.12$) $ \times 10^{-3}$ 1.3
Γ37  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}$  $0.03947$ $\pm0.00030$ 1.2
Γ38  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit \pi}^{0}}$  $0.01240$ $\pm0.00022$ 
Γ43  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$  $0.0280$ $\pm0.0018$ 1.1
Γ58  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{0}}$  $0.144$ $\pm0.006$ 2.2
Γ77  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}$2 ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$  $0.0822$ $\pm0.0014$ 1.1
Γ88  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$  $0.052$ $\pm0.006$ 
Γ94  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}$2 ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$  $0.043$ $\pm0.004$ 
Γ103  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \eta}}$  $0.0188$ $\pm0.0005$ 1.4
Γ117  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit \eta}}$  ($5.09$ $\pm0.13$) $ \times 10^{-3}$ 
Γ118  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit \omega}}$  $0.0111$ $\pm0.0006$ 
Γ119  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit \eta}^{\,'}{(958)}}$  ($9.49$ $\pm0.32$) $ \times 10^{-3}$ 
Γ133  ${{\mathit D}^{0}}$ $\rightarrow$ 3 ${{\mathit K}_S^0}$  ($7.5$ $\pm0.7$) $ \times 10^{-4}$ 1.4
Γ140  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$  ($1.454$ $\pm0.024$) $ \times 10^{-3}$ 1.4
Γ141  ${{\mathit D}^{0}}$ $\rightarrow$ 2 ${{\mathit \pi}^{0}}$  ($8.26$ $\pm0.25$) $ \times 10^{-4}$ 
Γ142  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$  $0.0149$ $\pm0.0007$ 2.3
Γ160  ${{\mathit D}^{0}}$ $\rightarrow$ 2 ${{\mathit \pi}^{+}}$2 ${{\mathit \pi}^{-}}$  ($7.56$ $\pm0.20$) $ \times 10^{-3}$ 
Γ189  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \pi}^{0}}$  ($6.3$ $\pm0.6$) $ \times 10^{-4}$ 1.1
Γ203  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \eta}^{\,'}{(958)}}{{\mathit \pi}^{0}}$  ($9.2$ $\pm1.0$) $ \times 10^{-4}$ 
Γ205  ${{\mathit D}^{0}}$ $\rightarrow$ 2 ${{\mathit \eta}}$  ($2.11$ $\pm0.19$) $ \times 10^{-3}$ 2.2
Γ209  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \eta}^{\,'}{(958)}}$  ($1.01$ $\pm0.19$) $ \times 10^{-3}$ 
Γ210  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}$  ($4.08$ $\pm0.06$) $ \times 10^{-3}$ 1.6
Γ211  ${{\mathit D}^{0}}$ $\rightarrow$ 2 ${{\mathit K}_S^0}$  ($1.41$ $\pm0.05$) $ \times 10^{-4}$ 1.1
Γ212  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}$  ($3.3$ $\pm0.5$) $ \times 10^{-3}$ 1.1
Γ223  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$  ($2.17$ $\pm0.34$) $ \times 10^{-3}$ 1.1
Γ284  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit \phi}}{{\mathit \gamma}}$  ($2.81$ $\pm0.19$) $ \times 10^{-5}$ 
Γ288  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$  ($1.50$ $\pm0.07$) $ \times 10^{-4}$ 3.0
Γ295  ${{\mathit D}^{0}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{0}}$  ($3.06$ $\pm0.16$) $ \times 10^{-4}$ 1.4
Γ355  ${{\mathit D}^{0}}$ $\rightarrow$ Unaccounted decay modes $0.350$ $\pm0.013$ 1.1

 
An overall fit to 3 branching ratios uses 3 measurements and one constraint to determine 4 parameters. The overall fit has a $\chi {}^{2}$ = 0.0 for 0 degrees of freedom.
 
The following off-diagonal array elements are the correlation coefficients <$\mathit \delta $x$_{i}$~$\delta $x$_{j}$> $/$ ($\mathit \delta $x$_{i}\cdot{}\delta $x$_{j}$), in percent, from the fit to parameters ${{\mathit p}_{{i}}}$, including the branching fractions, $\mathit x_{i}$ =$\Gamma _{i}$ $/$ $\Gamma _{total}$. The fit constrains the ${{\mathit x}_{{i}}}$ whose labels appear in this array to sum to one.
 
 x1  100
 x2   100
 x3    100
 x4     100
   x1  x2  x3  x4
 
  Mode Fraction (Γi / Γ)Scale factor

Γ1  ${{\mathit D}^{0}}$ $\rightarrow$ 0-prongs $0.15$ $\pm0.06$ 
Γ2  ${{\mathit D}^{0}}$ $\rightarrow$ 2-prongs $0.71$ $\pm0.06$ 
Γ3  ${{\mathit D}^{0}}$ $\rightarrow$ 4-prongs $0.146$ $\pm0.005$ 
Γ4  ${{\mathit D}^{0}}$ $\rightarrow$ 6-prongs ($6.5$ $\pm1.3$) $ \times 10^{-4}$