De Moivre–Laplace theorem





In probability theory, the de Moivre–Laplace theorem, which is a special case of the central limit theorem, states that the normal distribution may be used as an approximation to the binomial distribution under certain conditions. In particular, the theorem shows that the probability mass function of the random number of "successes" observed in a series of $$n$$ independent Bernoulli trials, each having probability $$p$$ of success (a binomial distribution with $$n$$ trials), converges to the probability density function of the normal distribution with expectation $$np$$ and standard deviation $\sqrt{np(1-p)}$, as $$n$$ grows large, assuming $$p$$ is not $$0$$ or $$1$$.

The theorem appeared in the second edition of The Doctrine of Chances by Abraham de Moivre, published in 1738. Although de Moivre did not use the term "Bernoulli trials", he wrote about the probability distribution of the number of times "heads" appears when a coin is tossed 3600 times.

This is one derivation of the particular Gaussian function used in the normal distribution.

It is a special case of the central limit theorem because a Bernoulli process can be thought of as the drawing of independent random variables from a bimodal discrete distribution with non-zero probability only for values 0 and 1. In this case, the binomial distribution models the number of successes (i.e., the number of 1s), whereas the central limit theorem states that, given sufficiently large n, the distribution of the sample means will be approximately normal. However, because in this case the fraction of successes (i.e., the number of 1s divided by the number of trials, n) is equal to the sample mean, the distribution of the fractions of successes (described by the binomial distribution divided by the constant n) and the distribution of the sample means (approximately normal with large n due to the central limit theorem) are equivalent.

Theorem
As n grows large, for k in the neighborhood of np we can approximate
 * $${n \choose k}\, p^k q^{n-k} \simeq \frac{1}{\sqrt{2 \pi npq}}\,e^{-\frac{(k-np)^2}{2npq}}, \qquad p+q=1,\ p, q > 0$$

in the sense that the ratio of the left-hand side to the right-hand side converges to 1 as n → ∞.

Proof
The theorem can be more rigorously stated as follows: $$\left(X\!\,-\!\, np\right)\!/\!\sqrt{npq}$$, with $$\textstyle X$$ a binomially distributed random variable, approaches the standard normal as $$n\!\to\!\infty$$, with the ratio of the probability mass of $$X$$ to the limiting normal density being 1. This can be shown for an arbitrary nonzero and finite point $$c$$. On the unscaled curve for $$X$$, this would be a point $$k$$ given by


 * $$k=np+c\sqrt{npq}$$

For example, with $$c$$ at 3, $$k$$ stays 3 standard deviations from the mean in the unscaled curve.

The normal distribution with mean $$\mu$$ and standard deviation $$\sigma$$ is defined by the differential equation (DE)


 * $$f'\!(x)\!=\!-\!\,\frac{x-\mu}{\sigma^2}f(x)$$ with an initial condition set by the probability axiom $$\int_{-\infty}^{\infty}\!f(x)\,dx\!=\!1$$.

The binomial distribution limit approaches the normal if the binomial satisfies this DE. As the binomial is discrete the equation starts as a difference equation whose limit morphs to a DE. Difference equations use the discrete derivative, $$\textstyle p(k\!+\!1)\!-\!p(k)$$, the change for step size 1. As $$\textstyle n\!\to\!\infty$$, the discrete derivative becomes the continuous derivative. Hence the proof need show only that, for the unscaled binomial distribution,


 * $$\frac{f'\!(x)}{f\!(x)}\!\cdot\! \left(-\frac{\sigma^2}{x-\mu}\right) \!\to\! 1$$ as $$ n\!\to\!\infty$$.

The required result can be shown directly:



\begin{align} \frac{f'\!(x)}{f\!(x)}\frac{npq}{np\!\,-\!\,k}\!&=\frac{p\left(n, k + 1\right) - p\left(n, k\right)}{p\left(n, k\right)}\frac{\sqrt{npq}}{-c} \\ &= \frac{np - k -q}{kq+q}\frac{\sqrt{npq}}{-c} \\ &= \frac{-c\sqrt{npq} -q}{npq + cq\sqrt{npq}+q}\frac{\sqrt{npq}}{-c} \\ & \to 1 \end{align} $$

The last holds because the term $$-cnpq$$ dominates both the denominator and the numerator as $$n\!\to\!\infty$$.

As $$\textstyle k$$ takes just integral values, the constant $$\textstyle c$$ is subject to a rounding error. However, the maximum of this error, $$\textstyle {0.5}/\!\sqrt{npq}$$, is a vanishing value.

Alternative proof
The proof consists of transforming the left-hand side (in the statement of the theorem) to the right-hand side by three approximations.

First, according to Stirling's formula, the factorial of a large number n can be replaced with the approximation


 * $$n! \simeq n^n e^{-n}\sqrt{2 \pi n}\qquad \text{as } n \to \infty.$$

Thus


 * $$\begin{align}{n \choose k} p^k q^{n-k} & = \frac{n!}{k!(n-k)!} p^k q^{n-k} \\& \simeq \frac{n^n e^{-n}\sqrt{2\pi n} }{k^ke^{-k}\sqrt{2\pi k} (n-k)^{n-k}e^{-(n-k)}\sqrt{2\pi (n-k)}} p^k q^{n-k}\\&=\sqrt{\frac{n}{2\pi k\left(n-k\right)}}\frac{n^n}{k^k\left(n-k\right)^{n-k}}p^kq^{n-k}\\&=\sqrt{\frac{n}{2\pi k\left(n-k\right)}}\left(\frac{np}{k}\right)^k\left(\frac{nq}{n-k}\right)^{n-k}\end{align}$$

Next, the approximation $$\tfrac{k}{n} \to p$$ is used to match the root above to the desired root on the right-hand side.


 * $$\begin{align}{n \choose k} p^k q^{n-k} & \simeq \sqrt{\frac{1}{2\pi n\frac{k}{n}\left(1-\frac{k}{n}\right)}}\left(\frac{np}{k}\right)^{k} \left(\frac{nq}{n-k}\right)^{n-k}\\&\simeq\frac{1}{\sqrt {2\pi npq}}\left(\frac{np}{k}\right)^{k} \left(\frac{nq}{n-k}\right)^{n-k} \qquad p+q=1\\ \end{align}$$

Finally, the expression is rewritten as an exponential and the Taylor Series approximation for ln(1+x) is used:


 * $$ \ln\left(1+x\right)\simeq x-\frac{x^2}{2}+\frac{x^3}{3}-\cdots$$

Then


 * $$\begin{align}{n \choose k} p^k q^{n-k} &\simeq \frac{1}{\sqrt {2\pi npq}}\exp\left\{\ln \left( \left(\frac{np}{k}\right)^{k} \right)+\ln \left( \left(\frac{nq}{n-k}\right)^{n-k}\right)\right\}\\ &=\frac{1}{\sqrt {2\pi npq}}\exp\left\{-k\ln\left(\frac{k}{np}\right)+(k-n)\ln \left(\frac{n-k}{nq}\right)\right\}\\&=\frac{1}{\sqrt {2\pi npq}}\exp\left\{-k\ln\left(\frac{np+x\sqrt{npq}}{np}\right)+(k-n)\ln \left(\frac{n-np-x\sqrt{npq}}{nq}\right)\right\}\\&=\frac{1}{\sqrt {2\pi npq}}\exp\left\{-k\ln\left({1+x\sqrt\frac{q}{np}}\right)+(k-n)\ln \left({1-x\sqrt\frac{p}{nq}}\right)\right\}\qquad p+q=1\\&=\frac{1}{\sqrt {2\pi npq}}\exp\left\{-k\left({x\sqrt\frac{q}{np}}-\frac{x^2q}{2np}+\cdots\right)+(k-n) \left({-x\sqrt\frac{p}{nq}-\frac{x^2p}{2nq}}-\cdots\right)\right\}\\&=\frac{1}{\sqrt {2\pi npq}}\exp\left\{\left(-np-x\sqrt{npq}\right)\left({x\sqrt\frac{q}{np}}-\frac{x^2q}{2np}+\cdots\right)+\left(np+x\sqrt{npq}-n\right) \left(-x\sqrt\frac{p}{nq}-\frac{x^2p}{2nq}-\cdots\right)\right\}\\&=\frac{1}{\sqrt {2\pi npq}}\exp\left\{\left(-np-x\sqrt{npq}\right)\left(x\sqrt\frac{q}{np}-\frac{x^2q}{2np}+\cdots\right)-\left(nq-x\sqrt{npq}\right) \left(-x\sqrt\frac{p}{nq}-\frac{x^2p}{2nq}-\cdots\right)\right\}\\&=\frac{1}{\sqrt {2\pi npq}}\exp\left\{\left(-x\sqrt{npq}+\frac{1}{2}x^2q-x^2q+\cdots\right)+\left(x\sqrt{npq}+\frac{1}{2}x^2p-x^2p-\cdots\right) \right\}\\&=\frac{1}{\sqrt {2\pi npq}}\exp\left\{-\frac{1}{2}x^2q-\frac{1}{2}x^2p-\cdots\right\}\\&=\frac{1}{\sqrt {2\pi npq}}\exp\left\{-\frac{1}{2}x^2(p+q)-\cdots\right\}\\&\simeq\frac{1}{\sqrt {2\pi npq}}\exp\left\{-\frac{1}{2}x^2\right\}\\&=\frac{1}{\sqrt {2\pi npq}}e^\frac{-(k-np)^2}{2npq}\\ \end{align}$$

Each "$$\simeq$$" in the above argument is a statement that two quantities are asymptotically equivalent as n increases, in the same sense as in the original statement of the theorem—i.e., that the ratio of each pair of quantities approaches 1 as n → ∞.