Let \phi(x) denote the
standard normal probability density function \phi(x)=\frac{1}{\sqrt{2\pi}}e^{-\frac{x^2}{2}} with the
cumulative distribution function given by \Phi(x) = \int_{-\infty}^{x} \phi(t)\ \mathrm dt = \frac{1}{2} \left[ 1 + \operatorname{erf} \left(\frac{x}{\sqrt{2}}\right)\right], where "erf" is the
error function. Then the probability density function (pdf) of the skew-normal distribution with parameter \alpha is given by f(x) = 2\phi(x)\Phi(\alpha x). \, This distribution was first introduced by O'Hagan and Leonard (1976). Alternative forms to this distribution, with the corresponding quantile function, have been given by Ashour and Abdel-Hamid and by Mudholkar and Hutson. A stochastic process that underpins the distribution was described by Andel, Netuka and Zvara (1984). Both the distribution and its stochastic process underpinnings were consequences of the symmetry argument developed in Chan and Tong (1986), which applies to multivariate cases beyond normality, e.g. skew multivariate t distribution and others. The distribution is a particular case of a general class of distributions with probability density functions of the form f(x) = 2 \phi(x) \Phi(x) where \phi(\cdot) is any
PDF symmetric about zero and \Phi(\cdot) is any
CDF whose PDF is symmetric about zero. To add
location and
scale parameters to this, one makes the usual transform x\rightarrow\frac{x-\xi}{\omega}. One can verify that the normal distribution is recovered when \alpha = 0, and that the absolute value of the
skewness increases as the absolute value of \alpha increases. The distribution is right skewed if \alpha>0 and is left skewed if \alpha . The probability density function with location \xi, scale \omega, and parameter \alpha becomes f(x) = \frac{2}{\omega} \phi{\left(\frac{x-\xi}{\omega}\right)} \, \Phi{\left(\alpha \left(\frac{x-\xi}{\omega}\right)\right)}. The skewness ( \gamma_1 ) of the distribution is limited to slightly less than the interval (-1,1) . As has been shown, the mode (maximum) m_o of the distribution is unique. For general \alpha there is no analytic expression for m_o , but a quite accurate (numerical) approximation is: \begin{align} \delta &= \frac{\alpha}{\sqrt{1+\alpha^2}} \\ m_o (\alpha) &\approx \sqrt{\frac{2}{\pi}}\delta - \left(1-\frac{\pi}{4}\right) \frac{\left(\sqrt{\frac{2}{\pi}}\delta\right)^3}{1-\frac{2}{\pi}\delta^2} - \frac{\mathrm{sgn}(\alpha)}{2} e^{-\frac{2 \pi}} \\ \end{align} ==Estimation==