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Theorem (Lindeberg's central limit theorem)
Let
 be independent random variables with distribution functions
 , respectively, such that
 and
 , with at least one
 . Let
 and  Then the normalized partial sums
 converge in distribution to a random variable with normal distribution  (i.e. the normal convergence holds,) if the following Lindeberg condition is satisfied:
Corollary 1 (Lyapunov's central limit theorem)
If the Lyapunov condition
is satisfied for some  , the normal convergence holds.
Corollary 2
If
 are identically distributed random variables,  and
 , with
 , then the normal convergence holds; i.e.
 converges in distribution to a random variable with distribution  .
Reciprocal (Feller)
The reciprocal of Lindeberg's central limit theorem holds under the following additional assumption:
Historical remark
The normal distribution was historically called the law of errors. It was used by Gauss to model errors in astronomical observations, which is why it is usually referred to as the Gaussian distribution. Gauss derived the normal distribution, not as a limit of sums of independent random variables, but from the consideration of certain “natural” hypotheses for the distribution of errors; e.g. considering the arithmetic mean of the observations to be the “most probable” value of the quantity being observed.
Nowadays, the central limit theorem supports the use of normal distribution as a distribution of errors, since in many real situations it is possible to consider the error of an observation as the result of many independent small errors. There are, too, many situations which are not subject to observational errors, in which the use of the normal distribution can still be justified by the central limit theorem. For example, the distribution of heights of mature men of a certain age can be considered normal, since height can be seen as the sum of many small and independent effects.
The normal distribution did not have its origins with Gauss. It appeared, at least discretely, in the work of De Moivre, who proved the central limit theorem for the case of Bernoulli essays with p=1/2 (e.g. when the n-th random variable is the result of tossing a coin.)
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![$\displaystyle \frac{1}{s_n^{2+\delta}}\sum_{k=1}^n E\vert X_k-\mu_k\vert^{2+\delta} \xrightarrow[n\rightarrow\infty]{} 0$](http://images.planetmath.org:8080/cache/objects/3713/l2h/img11.png "$\displaystyle \frac{1}{s_n^{2+\delta}}\sum_{k=1}^n E\vert X_k-\mu_k\vert^{2+\delta} \xrightarrow[n\rightarrow\infty]{} 0$")
![$\displaystyle \max_{1\leq k\leq n} \left(\frac{\sigma_k^2}{s_n^2}\right)\xrightarrow[n\rightarrow\infty]{} 0.$](http://images.planetmath.org:8080/cache/objects/3713/l2h/img19.png "$\displaystyle \max_{1\leq k\leq n} \left(\frac{\sigma_k^2}{s_n^2}\right)\xrightarrow[n\rightarrow\infty]{} 0.$")