An overall fit to 31 branching ratios uses 41 measurements and one constraint to determine 17 parameters. The overall fit has a $\chi {}^{2}$ = 62.8 for 25 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.
 x17  100
 x18   100
 x25    100
 x29     100
 x40      100
 x49       100
 x51        100
 x77         100
 x86          100
 x102           100
 x103            100
 x110             100
 x112              100
 x138               100
 x139                100
 x140                 100
 x183                  100
   x17  x18  x25  x29  x40  x49  x51  x77  x86  x102  x103  x110  x112  x138  x139  x140  x183
  Mode Fraction (Γi / Γ)Scale factor

Γ17  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\overline{\mathit K}}^{0}}{{\mathit \mu}^{+}}{{\mathit \nu}_{{\mu}}}$  $0.0876$ $\pm0.0019$ 
Γ18  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit e}^{+}}{{\mathit \nu}_{{e}}}$  $0.0402$ $\pm0.0018$ 3.2
Γ25  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\overline{\mathit K}}^{*}{(892)}^{0}}{{\mathit e}^{+}}{{\mathit \nu}_{{e}}}$  $0.0540$ $\pm0.0010$ 1.1
Γ29  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\overline{\mathit K}}^{*}{(892)}^{0}}{{\mathit \mu}^{+}}{{\mathit \nu}_{{\mu}}}$  $0.0527$ $\pm0.0015$ 1.0
Γ40  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit \rho}^{0}}{{\mathit e}^{+}}{{\mathit \nu}_{{e}}}$  $0.00218$ ${}^{+0.00017}_{-0.00025}$ 
Γ49  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit \pi}^{+}}$  $0.01562$ $\pm0.00031$ 1.7
Γ51  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}$2 ${{\mathit \pi}^{+}}$  $0.0938$ $\pm0.0016$ 1.6
Γ77  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}$3 ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$  $0.0057$ $\pm0.0005$ 1.1
Γ86  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit \pi}^{+}}{{\mathit \pi}^{0}}$  $0.001247$ $\pm0.000033$ 
Γ102  ${{\mathit D}^{+}}$ $\rightarrow$ 3 ${{\mathit \pi}^{+}}$2 ${{\mathit \pi}^{-}}$  $0.00166$ $\pm0.00016$ 1.1
Γ103  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit \eta}}{{\mathit \pi}^{+}}$  $0.00377$ $\pm0.00009$ 
Γ110  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit \eta}^{\,'}{(958)}}{{\mathit \pi}^{+}}$  $0.00497$ $\pm0.00019$ 
Γ112  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{+}}$  $0.00304$ $\pm0.00009$ 2.2
Γ138  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{0}}$  ($2.08$ $\pm0.21$) $ \times 10^{-4}$ 1.4
Γ139  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \eta}}$  ($1.25$ $\pm0.16$) $ \times 10^{-4}$ 1.1
Γ140  ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \eta}^{\,'}{(958)}}$  ($1.85$ $\pm0.20$) $ \times 10^{-4}$ 
Γ183  ${{\mathit D}^{+}}$ $\rightarrow$ Unaccounted decay modes $0.633$ $\pm0.004$ 1.3