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Fisher transformation
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==Definition== Given a set of ''N'' bivariate sample pairs (''X''<sub>''i''</sub>, ''Y''<sub>''i''</sub>), ''i'' = 1, ..., ''N'', the [[Pearson product-moment correlation coefficient|sample correlation coefficient]] ''r'' is given by :<math>r = \frac{\operatorname{cov}(X,Y)}{\sigma_X \sigma_Y} = \frac{\sum ^N _{i=1}(X_i - \bar{X})(Y_i - \bar{Y})}{\sqrt{\sum ^N _{i=1}(X_i - \bar{X})^2} \sqrt{\sum ^N _{i=1}(Y_i - \bar{Y})^2}}.</math> Here <math>\operatorname{cov}(X,Y)</math> stands for the [[covariance]] between the variables <math>X</math> and <math>Y</math> and <math>\sigma</math> stands for the [[standard deviation]] of the respective variable. Fisher's z-transformation of ''r'' is defined as :<math>z = {1 \over 2}\ln\left({1+r \over 1-r}\right) = \operatorname{artanh}(r),</math> where "ln" is the [[natural logarithm]] function and "artanh" is the [[inverse hyperbolic function|inverse hyperbolic tangent function]]. If (''X'', ''Y'') has a [[bivariate normal distribution]] with correlation Ο and the pairs (''X''<sub>''i''</sub>, ''Y''<sub>''i''</sub>) are [[Independent and identically distributed random variables|independent and identically distributed]], then ''z'' is approximately [[normal distribution|normally distributed]] with mean :<math>{1 \over 2}\ln\left({{1+\rho} \over {1-\rho}}\right),</math> and a standard deviation which does not depend on the value of the correlation rho (i.e., a [[Variance-stabilizing transformation]]) :<math>{1 \over \sqrt{N-3}},</math> where ''N'' is the sample size, and Ο is the true correlation coefficient. This transformation, and its inverse :<math>r = \frac{\exp(2z)-1}{\exp(2z)+1} = \operatorname{tanh}(z),</math> can be used to construct a large-sample [[confidence interval]] for ''r'' using standard normal theory and derivations. See also application to [[partial correlation]].
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