Lindeberg's condition

In probability theory, Lindeberg's condition is a sufficient condition (and under certain conditions also a necessary condition) for the central limit theorem (CLT) to hold for a sequence of independent random variables.

[1][2][3] Unlike the classical CLT, which requires that the random variables in question have finite variance and be both independent and identically distributed, Lindeberg's CLT only requires that they have finite variance, satisfy Lindeberg's condition, and be independent.

It is named after the Finnish mathematician Jarl Waldemar Lindeberg.

be a probability space, and

, be independent random variables defined on that space.

Assume the expected values

exist and are finite.

If this sequence of independent random variables

satisfies Lindeberg's condition: for all

ε > 0

, where 1{…} is the indicator function, then the central limit theorem holds, i.e. the random variables converge in distribution to a standard normal random variable as

Lindeberg's condition is sufficient, but not in general necessary (i.e. the inverse implication does not hold in general).

However, if the sequence of independent random variables in question satisfies then Lindeberg's condition is both sufficient and necessary, i.e. it holds if and only if the result of central limit theorem holds.

Feller's theorem can be used as an alternative method to prove that Lindeberg's condition holds.

, the theorem states

This theorem can be used to disprove the central limit theorem holds for

by using proof by contradiction.

This procedure involves proving that Lindeberg's condition fails for

Because the Lindeberg condition implies

, it guarantees that the contribution of any individual random variable

is arbitrarily small, for sufficiently large values of

Consider the following informative example which satisfies the Lindeberg condition.

ξ

be a sequence of zero mean, variance 1 iid random variables and

a non-random sequence satisfying:

Now, define the normalized elements of the linear combination:

ξ

which satisfies the Lindeberg condition:

ξ

is finite so by DCT and the condition on the