Then the distribution of ''Z''
''n'' Converges towards the
Standard Normal Distribution N(0,1)
as ''n'' approaches ∞ (this is of N(0,1), then for every
Real Number ''z'', we have
:
or, equivalently,
:
where
:
is the
Sample Mean .
For a theorem of such fundamental importance to
Statistics and
Applied Probability , the central limit theorem has a remarkably simple proof using
Characteristic Functions . It is similar to the proof of a (weak)
Law Of Large Numbers . For any random variable, ''Y'', with zero
Mean and unit variance (var(''Y'') = 1), the characteristic function of ''Y'' is, by
Taylor's Theorem ,
:
where ''o'' (''t
2'' ) is "
Little O Notation " for some function of ''t'' that goes to zero more rapidly than ''t
2''. Letting ''Y''
''i'' be (''X''
''i'' − μ)/σ, the standardised value of ''X''
''i'', it is easy to see that the standardised mean of the observations
X1,
X2, ...,
X''n'' is just
:
By simple properties of characteristic functions, the characteristic function of ''Z''
''n'' is
:
But, this limit is just the characteristic function of a standard normal distribution, N(0,1), and the central limit theorem follows from the
Lévy Continuity Theorem , which confirms that the
Convergence of characteristic functions implies convergence in distribution.
If the third central
Moment E((''X''
1 − μ)
3) exists and is finite, then the above convergence is
Uniform and the speed of convergence is at least on the order of 1/''n''
½ (see
Berry-Esséen Theorem ).
Pictures of a distribution being "smoothed out" by
Summation (showing original distribution and three subsequent
Convolution s):
(See
Illustration Of The Central Limit Theorem for further details on these images.)
An equivalent formulation of this limit theorem starts with ''A''
''n'' = (''X''
1 + ... + ''X''
''n'') / ''n'' which can be interpreted as the mean of a
Random Sample of size ''n''. The expected value of ''A''
''n'' is μ and the standard deviation is σ / ''n''
½. If we standardize ''A''
''n'' by setting ''Z''
''n'' = (''A''
''n'' - μ) / (σ / ''n''
½), we obtain the same variable ''Z''
''n'' as above, and it approaches a standard normal distribution.
Note the following apparent "
Paradox ": by adding many independent identically distributed ''positive'' variables, one gets approximately a normal distribution. But for every normally distributed variable, the probability that it is negative is non-zero! How is it possible to get negative numbers from adding only positives?
The reason is simple: the theorem applies to terms centered about the mean. Without that standardization, the distribution would, as intuition suggests, escape away to infinity.
The Central Limit Theorem, as an approximation for a finite number of observations, provides a reasonable approximation only when close to the peak of the normal distribution; it requires a very large number of observations to stretch into the tails.
The Central Limit theorem also applies to sums of independent and identical s is still a
Discrete Random Variable , so that we are confronted to a
Series of
Discrete Random Variable s whose probability distribution converges towards a
Probability Density Function corresponding to a continuous variable (namely the
Normal Distribution ). This means that if we build an
Organigram of the realisations of the sum of ''n'' independent identical discrete variables, the curve that joins the centers of the upper faces of the rectangles forming the organigram converges toward a gaussian curve as ''n'' approaches
. The
Binomial Distribution article details such an application of the central limit theorem in the simple case of a discrete variable taking only two possible values.
The
Density of the sum of two or more independent variables is the
Convolution of their densities (if these densities exist).
Thus the central limit theorem can be interpreted as a statement about the properties of density functions under convolution:
the convolution of a number of density functions tends to the normal density as the number of density functions increases without bound,
under the conditions stated above.
Since the
Characteristic Function of a convolution is the product of the characteristic functions of the densities involved,
the central limit theorem has yet another restatement:
the product of the characteristic functions of a number of density functions tends to the characteristic function of the normal density as the number of density functions increases without bound,
under the conditions stated above.
An equivalent statement can be made about
Fourier Transform s,
since the characteristic function is essentially a Fourier transform.
The central limit theorem tells us what to expect about the sum of independent random variables, but what about the product? Well, the
Logarithm of a product is simply the sum of the logs of the factors, so the log of a product of random variables tends to have a normal distribution, which makes the product itself have a
Log-normal Distribution . Many physical quantities (especially mass or length, which are a matter of scale and cannot be negative) are the product of different
Random factors, so they follow a log-normal distribution.
See also
Lyapunov's Central Limit Theorem .
Let ''X''
''n'' be a sequence of independent random variables defined on the same probability space. Assume that ''X''
''n'' has finite expected value μ
''n'' and finite standard deviation σ
''n''. We define
:
Assume that the third central moments