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Taylor expansions for the moments of functions of random variables
Concept in probability theory From Wikipedia, the free encyclopedia
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In probability theory, it is possible to approximate the moments of a function f of a random variable X using Taylor expansions, provided that f is sufficiently differentiable and that the moments of X are finite.
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A simulation-based alternative to this approximation is the application of Monte Carlo simulations.
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First moment
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Given and , the mean and the variance of , respectively,[1] a Taylor expansion of the expected value of can be found via
Since the second term vanishes. Also, is . Therefore,
- .
It is possible to generalize this to functions of more than one variable using multivariate Taylor expansions. For example,[2]
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Second moment
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Similarly,[1]
The above is obtained using a second order approximation, following the method used in estimating the first moment. It will be a poor approximation in cases where is highly non-linear. This is a special case of the delta method.
Indeed, we take .
With , we get . The variance is then computed using the formula .
An example is,[2]
The second order approximation, when X follows a normal distribution, is:[3]
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First product moment
To find a second-order approximation for the covariance of functions of two random variables (with the same function applied to both), one can proceed as follows. First, note that . Since a second-order expansion for has already been derived above, it only remains to find . Treating as a two-variable function, the second-order Taylor expansion is as follows:
Taking expectation of the above and simplifying—making use of the identities and —leads to . Hence,
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Random vectors
If X is a random vector, the approximations for the mean and variance of are given by[4]
Here and denote the gradient and the Hessian matrix respectively, and is the covariance matrix of X.
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See also
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Further reading
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