Bernoulli distribution

In probability theory and statistics, the Bernoulli distribution, named after Swiss mathematician Jacob Bernoulli, is the discrete probability distribution of a random variable which takes the value 1 with probability ${\displaystyle p}$ and the value 0 with probability ${\displaystyle q=1-p}$. Less formally, it can be thought of as a model for the set of possible outcomes of any single experiment that asks a yes–no question. Such questions lead to outcomes that are Boolean-valued: a single bit whose value is success/yes/true/one with probability p and failure/no/false/zero with probability q. It can be used to represent a (possibly biased) coin toss where 1 and 0 would represent "heads" and "tails", respectively, and p would be the probability of the coin landing on heads (or vice versa where 1 would represent tails and p would be the probability of tails). In particular, unfair coins would have ${\displaystyle p\neq 1/2.}$

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Bernoulli distribution

In probability theory and statistics, the Bernoulli distribution, named after Swiss mathematician Jacob Bernoulli, is the discrete probability distribution of a random variable which takes the value 1 with probability ${\displaystyle p}$ and the value 0 with probability ${\displaystyle q=1-p}$. Less formally, it can be thought of as a model for the set of possible outcomes of any single experiment that asks a yes–no question. Such questions lead to outcomes that are Boolean-valued: a single bit whose value is success/yes/true/one with probability p and failure/no/false/zero with probability q. It can be used to represent a (possibly biased) coin toss where 1 and 0 would represent "heads" and "tails", respectively, and p would be the probability of the coin landing on heads (or vice versa where 1 would represent tails and p would be the probability of tails). In particular, unfair coins would have ${\displaystyle p\neq 1/2.}$

The Bernoulli distribution is a special case of the binomial distribution where a single trial is conducted (so n would be 1 for such a binomial distribution). It is also a special case of the two-point distribution, for which the possible outcomes need not be 0 and 1.

Properties

Bernoulli distribution

If ${\displaystyle X}$ is a random variable with a Bernoulli distribution, then:

${\displaystyle {\begin{aligned}\Pr(X{=}1)&=p,\\\Pr(X{=}0)&=q=1-p.\end{aligned}}}$

The probability mass function ${\displaystyle f}$ of this distribution, over possible outcomes k, is

${\displaystyle f(k;p)={\begin{cases}p&{\text{if }}k=1,\\q=1-p&{\text{if }}k=0.\end{cases}}}$

${\displaystyle f(k;p)=p^{k}(1-p)^{1-k}\quad {\text{for }}k\in \{0,1\}}$

${\displaystyle f(k;p)=pk+(1-p)(1-k)\quad {\text{for }}k\in \{0,1\}.}$

The Bernoulli distribution is a special case of the binomial distribution with ${\displaystyle n=1.}$

The kurtosis goes to infinity for high and low values of ${\displaystyle p,}$ but for ${\displaystyle p=1/2}$ the two-point distributions including the Bernoulli distribution have a lower excess kurtosis, namely −2, than any other probability distribution.

The Bernoulli distributions for ${\displaystyle 0\leq p\leq 1}$ form an exponential family.

The maximum likelihood estimator of ${\displaystyle p}$ based on a random sample is the sample mean.

The probability mass distribution function of a Bernoulli experiment along with its corresponding cumulative distribution function

Mean

Bernoulli distribution

The expected value of a Bernoulli random variable ${\displaystyle X}$ is

This is because for a Bernoulli distributed random variable ${\displaystyle X}$ with ${\displaystyle \Pr(X{=}1)=p}$ and ${\textstyle \Pr(X{=}0)=q}$ we find

${\displaystyle {\begin{aligned}\operatorname {E} [X]&=\Pr(X{=}1)\cdot 1+\Pr(X{=}0)\cdot 0\\[1ex]&=p\cdot 1+q\cdot 0\\[1ex]&=p.\end{aligned}}}$

Variance

Bernoulli distribution

The variance of a Bernoulli distributed ${\displaystyle X}$ is

${\displaystyle \operatorname {Var} [X]=pq=p(1-p)}$

${\displaystyle {\begin{aligned}\operatorname {E} [X^{2}]&=\Pr(X{=}1)\cdot 1^{2}+\Pr(X{=}0)\cdot 0^{2}\\&=p\cdot 1^{2}+q\cdot 0^{2}\\&=p=\operatorname {E} [X]\end{aligned}}}$

${\displaystyle {\begin{aligned}\operatorname {Var} [X]&=\operatorname {E} [X^{2}]-\operatorname {E} [X]^{2}=\operatorname {E} [X]-\operatorname {E} [X]^{2}\\[1ex]&=p-p^{2}=p(1-p)=pq\end{aligned}}}$

With this result it is easy to prove that, for any Bernoulli distribution, its variance will have a value inside ${\displaystyle [0,1/4]}$.

Skewness

Bernoulli distribution

The skewness is ${\displaystyle {\frac {q-p}{\sqrt {pq}}}={\frac {1-2p}{\sqrt {pq}}}}$. When we take the standardized Bernoulli distributed random variable ${\displaystyle {\frac {X-\operatorname {E} [X]}{\sqrt {\operatorname {Var} [X]}}}}$ we find that this random variable attains ${\displaystyle {\frac {q}{\sqrt {pq}}}}$ with probability ${\displaystyle p}$ and attains ${\displaystyle -{\frac {p}{\sqrt {pq}}}}$ with probability ${\displaystyle q}$. Thus we get

${\displaystyle {\begin{aligned}\gamma {1}&=\operatorname {E} \left[\left({\frac {X-\operatorname {E} [X]}{\sqrt {\operatorname {Var} [X]}}}\right)^{3}\right]\\&=p\cdot \left({\frac {q}{\sqrt {pq}}}\right)^{3}+q\cdot \left(-{\frac {p}{\sqrt {pq}}}\right)^{3}\\&={\frac {1}{{\sqrt {pq}}^{3}}}\left(pq^{3}-qp^{3}\right)\\&={\frac {pq}{{\sqrt {pq}}^{3}}}(q^{2}-p^{2})\\&={\frac {(1-p)^{2}-p^{2}}{\sqrt {pq}}}\\&={\frac {1-2p}{\sqrt {pq}}}={\frac {q-p}{\sqrt {pq}}}.\end{aligned}}}$

Higher moments and cumulants

Bernoulli distribution

The raw moments are all equal because ${\displaystyle 1^{k}=1}$ and ${\displaystyle 0^{k}=0}$.

${\displaystyle \operatorname {E} [X^{k}]=\Pr(X{=}1)\cdot 1^{k}+\Pr(X{=}0)\cdot 0^{k}=p\cdot 1+q\cdot 0=p=\operatorname {E} [X].}$

The central moment of order ${\displaystyle k}$ is given by ${\displaystyle \mu {k}=(1-p)(-p)^{k}+p(1-p)^{k}.}$ The first six central moments are ${\displaystyle {\begin{aligned}\mu {1}&=0,\\\mu {2}&=p(1-p),\\\mu {3}&=p(1-p)(1-2p),\\\mu {4}&=p(1-p)(1-3p(1-p)),\\\mu {5}&=p(1-p)(1-2p)(1-2p(1-p)),\\\mu {6}&=p(1-p)(1-5p(1-p)(1-p(1-p))).\end{aligned}}}$ The higher central moments can be expressed more compactly in terms of ${\displaystyle \mu {2}}$ and ${\displaystyle \mu {3}}$ ${\displaystyle {\begin{aligned}\mu {4}&=\mu {2}(1-3\mu {2}),\\\mu {5}&=\mu {3}(1-2\mu {2}),\\\mu {6}&=\mu {2}(1-5\mu {2}(1-\mu {2})).\end{aligned}}}$ The first six cumulants are ${\displaystyle {\begin{aligned}\kappa {1}&=p,\\\kappa {2}&=\mu {2},\\\kappa {3}&=\mu {3},\\\kappa {4}&=\mu {2}(1-6\mu {2}),\\\kappa {5}&=\mu {3}(1-12\mu {2}),\\\kappa {6}&=\mu {2}(1-30\mu {2}(1-4\mu {2})).\end{aligned}}}$

Entropy and Fisher's Information

Entropy

Entropy is a measure of uncertainty or randomness in a probability distribution. For a Bernoulli random variable ${\displaystyle X}$ with success probability ${\displaystyle p}$ and failure probability ${\displaystyle q=1-p}$, the entropy ${\displaystyle H(X)}$ is defined as:

${\displaystyle {\begin{aligned}H(X)&=\mathbb {E} {p}\ln {\frac {1}{\Pr(X)}}\\[1ex]&=-\Pr(X{=}0)\ln \Pr(X{=}0)-\Pr(X{=}1)\ln \Pr(X{=}1)\\[1ex]&=-(q\ln q+p\ln p).\end{aligned}}}$

The entropy is maximized when ${\displaystyle p=0.5}$, indicating the highest level of uncertainty when both outcomes are equally likely. The entropy is zero when ${\displaystyle p=0}$ or ${\displaystyle p=1}$, where one outcome is certain.

Fisher's Information

Fisher information measures the amount of information that an observable random variable ${\displaystyle X}$ carries about an unknown parameter ${\displaystyle p}$ upon which the probability of ${\displaystyle X}$ depends. For the Bernoulli distribution, the Fisher information with respect to the parameter ${\displaystyle p}$ is given by:

• The Likelihood Function for a Bernoulli random variable${\displaystyle X}$ is: ${\displaystyle L(p;X)=p^{X}(1-p)^{1-X}}$ This represents the probability of observing ${\displaystyle X}$ given the parameter ${\displaystyle p}$. • The Log-Likelihood Function is: ${\displaystyle \ln L(p;X)=X\ln p+(1-X)\ln(1-p)}$ • The Score Function (the first derivative of the log-likelihood with respect to ${\displaystyle p}$ is: ${\displaystyle {\frac {\partial }{\partial p}}\ln L(p;X)={\frac {X}{p}}-{\frac {1-X}{1-p}}}$ • The second derivative of the log-likelihood function is: ${\displaystyle {\frac {\partial ^{2}}{\partial p^{2}}}\ln L(p;X)=-{\frac {X}{p^{2}}}-{\frac {1-X}{(1-p)^{2}}}}$ • Fisher information is calculated as the negative expected value of the second derivative of the log-likelihood:${\displaystyle {\begin{aligned}I(p)=-E\left[{\frac {\partial ^{2}}{\partial p^{2}}}\ln L(p;X)\right]=-\left(-{\frac {p}{p^{2}}}-{\frac {1-p}{(1-p)^{2}}}\right)={\frac {1}{p(1-p)}}={\frac {1}{pq}}\end{aligned}}}$

It is maximized when ${\displaystyle p=0.5}$, reflecting maximum uncertainty and thus maximum information about the parameter ${\displaystyle p}$.

Related distributions

Bernoulli distribution

• If ${\displaystyle X{1},\dots ,X{n}}$ are independent, identically distributed (i.i.d.) random variables, all Bernoulli trials with success probability p, then their sum is distributed according to a binomial distribution with parameters n and p: ${\displaystyle \sum {k=1}^{n}X{k}\sim \operatorname {B} (n,p)}$ (binomial distribution).

The Bernoulli distribution is simply ${\displaystyle \operatorname {B} (1,p)}$, also written as ${\textstyle \mathrm {Bernoulli} (p).}$

• The categorical distribution is the generalization of the Bernoulli distribution for variables with any constant number of discrete values. • The Beta distribution is the conjugate prior of the Bernoulli distribution. • The geometric distribution models the number of independent and identical Bernoulli trials needed to get one success. • If ${\textstyle Y\sim \mathrm {Bernoulli} \left({\frac {1}{2}}\right)}$, then ${\textstyle 2Y-1}$ has a Rademacher distribution.

Author's mention

Bernoulli distribution

• Abhirath, dwivedi; Kotz, Samuel; Kemp, Adrienne W. (1993). Univariate Discrete Distributions (2nd ed.). Wiley. ISBN 0-471-54897-9. • Peatman, John G. (1963). Introduction to Applied Statistics. New York: Harper & Row. pp. 162–171.