Empirical Distribution Function

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## Definition

## Small-sample properties

## Asymptotic properties

## See also

## References

## Further reading

## External links

This article uses material from the Wikipedia page available here. It is released under the Creative Commons Attribution-Share-Alike License 3.0.

Empirical Distribution Function

In statistics, an **empirical distribution function** is the distribution function associated with the empirical measure of a sample. This cumulative distribution function is a step function that jumps up by 1/*n* at each of the *n* data points. Its value at any specified value of the measured variable is the fraction of observations of the measured variable that are less than or equal to the specified value.

The empirical distribution function is an estimate of the cumulative distribution function that generated the points in the sample. It converges with probability 1 to that underlying distribution, according to the Glivenko-Cantelli theorem. A number of results exist to quantify the rate of convergence of the empirical distribution function to the underlying cumulative distribution function.

Let (*X*_{1}, ..., *X*_{n}) be independent, identically distributed real random variables with the common cumulative distribution function *F*(*t*). Then the **empirical distribution function** is defined as^{[1]}^{[2]}

where is the indicator of event *A*. For a fixed *t*, the indicator is a Bernoulli random variable with parameter *p* = *F*(*t*); hence is a binomial random variable with mean *nF*(*t*) and variance *nF*(*t*)(1 - *F*(*t*)). This implies that is an unbiased estimator for *F*(*t*).

However, in some textbooks, the definition is given as
^{[3]}^{[4]}

The mean of the empirical distribution is an unbiased estimator of the mean of the population distribution.

The variance of the empirical distribution times is an unbiased estimator of the variance of the population distribution.

Since the ratio (*n* + 1)/*n* approaches 1 as *n* goes to infinity, the asymptotic properties of the two definitions that are given above are the same.

By the strong law of large numbers, the estimator converges to *F*(*t*) as *n* -> ? almost surely, for every value of *t*:^{[1]}

thus the estimator is consistent. This expression asserts the pointwise convergence of the empirical distribution function to the true cumulative distribution function. There is a stronger result, called the Glivenko-Cantelli theorem, which states that the convergence in fact happens uniformly over *t*:^{[5]}

The sup-norm in this expression is called the Kolmogorov-Smirnov statistic for testing the goodness-of-fit between the empirical distribution and the assumed true cumulative distribution function *F*. Other norm functions may be reasonably used here instead of the sup-norm. For example, the L^{2}-norm gives rise to the Cramér-von Mises statistic.

The asymptotic distribution can be further characterized in several different ways. First, the central limit theorem states that *pointwise*, has asymptotically normal distribution with the standard rate of convergence:^{[1]}

This result is extended by the Donsker's theorem, which asserts that the *empirical process* , viewed as a function indexed by , converges in distribution in the Skorokhod space to the mean-zero Gaussian process , where *B* is the standard Brownian bridge.^{[5]} The covariance structure of this Gaussian process is

The uniform rate of convergence in Donsker's theorem can be quantified by the result known as the Hungarian embedding:^{[6]}

Alternatively, the rate of convergence of can also be quantified in terms of the asymptotic behavior of the sup-norm of this expression. Number of results exist in this venue, for example the Dvoretzky-Kiefer-Wolfowitz inequality provides bound on the tail probabilities of :^{[6]}

In fact, Kolmogorov has shown that if the cumulative distribution function *F* is continuous, then the expression converges in distribution to , which has the Kolmogorov distribution that does not depend on the form of *F*.

Another result, which follows from the law of the iterated logarithm, is that ^{[6]}

and

- Càdlàg functions
- Count data
- Distribution fitting
- Dvoretzky-Kiefer-Wolfowitz inequality
- Empirical probability
- Empirical process
- Estimating quantiles from a sample
- Frequency (statistics)
- Kaplan-Meier estimator for censored processes
- Survival function

- ^
^{a}^{b}^{c}van der Vaart, A.W. (1998).*Asymptotic statistics*. Cambridge University Press. p. 265. ISBN 0-521-78450-6. **^**PlanetMath Archived May 9, 2013, at the Wayback Machine.**^**Coles, S. (2001)*An Introduction to Statistical Modeling of Extreme Values*. Springer, p. 36, Definition 2.4. ISBN 978-1-4471-3675-0.**^**Madsen, H.O., Krenk, S., Lind, S.C. (2006)*Methods of Structural Safety*. Dover Publications. p. 148-149. ISBN 0486445976- ^
^{a}^{b}van der Vaart, A.W. (1998).*Asymptotic statistics*. Cambridge University Press. p. 266. ISBN 0-521-78450-6. - ^
^{a}^{b}^{c}van der Vaart, A.W. (1998).*Asymptotic statistics*. Cambridge University Press. p. 268. ISBN 0-521-78450-6.

- Shorack, G.R.; Wellner, J.A. (1986).
*Empirical Processes with Applications to Statistics*. New York: Wiley. ISBN 0-471-86725-X.

This article uses material from the Wikipedia page available here. It is released under the Creative Commons Attribution-Share-Alike License 3.0.

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