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Probability density function  
Cumulative distribution function  
Parameters  λ > 0 rate, or inverse scale 

Support  x ∈ [0, ∞) 
λ e^{−λx}  
CDF  1 − e^{−λx} 
Mean  λ^{−1} 
Median  λ^{−1} ln 2 
Mode  0 
Variance  λ^{−2} 
Skewness  2 
Ex. kurtosis  6 
Entropy  1 − ln(λ) 
MGF  
CF 
Probability density function  
Cumulative distribution function  
Parameters  λ > 0 rate, or inverse scale 

Support  x ∈ [0, ∞) 
λ e^{−λx}  
CDF  1 − e^{−λx} 
Mean  λ^{−1} 
Median  λ^{−1} ln 2 
Mode  0 
Variance  λ^{−2} 
Skewness  2 
Ex. kurtosis  6 
Entropy  1 − ln(λ) 
MGF  
CF 
In probability theory and statistics, the exponential distribution (a.k.a. radical exponential distribution) is the probability distribution that describes the time between events in a Poisson process, i.e. a process in which events occur continuously and independently at a constant average rate. It is the continuous analogue of the geometric distribution, and it has the key property of being memoryless. In addition to being used for the analysis of Poisson processes, it is found in various other contexts.
Note that the exponential distribution is not the same as the class of exponential families of distributions, which is a large class of probability distributions that includes the exponential distribution as one of its members, but also includes the normal distribution, binomial distribution, gamma distribution, Poisson, and many others.
The probability density function (pdf) of an exponential distribution is
Alternatively, this can be defined using the Heaviside step function, H(x).
Here λ > 0 is the parameter of the distribution, often called the rate parameter. The distribution is supported on the interval [0, ∞). If a random variable X has this distribution, we write X ~ Exp(λ).
The exponential distribution exhibits infinite divisibility.
The cumulative distribution function is given by
Alternatively, this can be defined using the Heaviside step function, H(x).
A commonly used alternative parameterization is to define the probability density function (pdf) of an exponential distribution as
where β > 0 is a scale parameter of the distribution and is the reciprocal of the rate parameter, λ, defined above. In this specification, β is a survival parameter in the sense that if a random variable X is the duration of time that a given biological or mechanical system manages to survive and X ~ Exp(β) then E[X] = β. That is to say, the expected duration of survival of the system is β units of time. The parameterisation involving the "rate" parameter arises in the context of events arriving at a rate λ, when the time between events (which might be modelled using an exponential distribution) has a mean of β = λ^{−1}.
The alternative specification is sometimes more convenient than the one given above, and some authors will use it as a standard definition. This alternative specification is not used here. Unfortunately this gives rise to a notational ambiguity. In general, the reader must check which of these two specifications is being used if an author writes "X ~ Exp(λ)", since either the notation in the previous (using λ) or the notation in this section (here, using β to avoid confusion) could be intended.
The mean or expected value of an exponentially distributed random variable X with rate parameter λ is given by
In light of the examples given above, this makes sense: if you receive phone calls at an average rate of 2 per hour, then you can expect to wait half an hour for every call.
The variance of X is given by
The moments of X, for n = 1, 2, ..., are given by
The median of X is given by
where ln refers to the natural logarithm. Thus the absolute difference between the mean and median is
in accordance with the medianmean inequality.
An exponentially distributed random variable T obeys the relation
When T is interpreted as the waiting time for an event to occur relative to some initial time, this relation implies that, if T is conditioned on a failure to observe the event over some initial period of time s, the distribution of the remaining waiting time is the same as the original unconditional distribution. For example, if an event has not occurred after 30 seconds, the conditional probability that occurrence will take at least 10 more seconds is equal to the unconditioned probability of observing the event more than 10 seconds relative to the initial time.
The exponential distributions and the geometric distributions are the only memoryless probability distributions.
The exponential distribution is consequently also necessarily the only continuous probability distribution that has a constant Failure rate.
The quantile function (inverse cumulative distribution function) for Exp(λ) is
The quartiles are therefore:
And as a consequence the interquartile range is ln(3)/λ.
The directed Kullback–Leibler divergence of Exp(λ) ('approximating' distribution) from Exp(λ_{0}) ('true' distribution) is given by
Among all continuous probability distributions with support [0, ∞) and mean μ, the exponential distribution with λ = 1/μ has the largest differential entropy. In other words, it is the maximum entropy probability distribution for a random variate X for which E[X] is fixed and greater than zero.^{[2]}
Let X_{1}, ..., X_{n} be independent exponentially distributed random variables with rate parameters λ_{1}, ..., λ_{n}. Then
is also exponentially distributed, with parameter
This can be seen by considering the complementary cumulative distribution function:
The index of the variable which achieves the minimum is distributed according to the law
Note that
is not exponentially distributed.
Suppose a given variable is exponentially distributed and the rate parameter λ is to be estimated.
The likelihood function for λ, given an independent and identically distributed sample x = (x_{1}, ..., x_{n}) drawn from the variable, is:
where:
is the sample mean.
The derivative of the likelihood function's logarithm is:
Consequently the maximum likelihood estimate for the rate parameter is:
The 100(1 − α)% confidence interval for the rate parameter of an exponential distribution is given by:^{[3]}
which is also equal to:
where χ^{2}_{p,v} is the 100(1 – p) percentile of the chi squared distribution with v degrees of freedom, n is the number of observations of interarrival times in the sample, and xbar is the sample average. A simple approximation to the exact interval endpoints can be derived using a normal approximation to the χ^{2}_{p,v} distribution. This approximation gives the following values for a 95% confidence interval:
This approximation may be acceptable for samples containing at least 15 to 20 elements.^{[4]}
The conjugate prior for the exponential distribution is the gamma distribution (of which the exponential distribution is a special case). The following parameterization of the gamma probability density function is useful:
The posterior distribution p can then be expressed in terms of the likelihood function defined above and a gamma prior:
Now the posterior density p has been specified up to a missing normalizing constant. Since it has the form of a gamma pdf, this can easily be filled in, and one obtains:
Here the parameter α can be interpreted as the number of prior observations, and β as the sum of the prior observations. The posterior mean here is :
A conceptually very simple method for generating exponential variates is based on inverse transform sampling: Given a random variate U drawn from the uniform distribution on the unit interval (0, 1), the variate
has an exponential distribution, where F^{ −1} is the quantile function, defined by
Moreover, if U is uniform on (0, 1), then so is 1 − U. This means one can generate exponential variates as follows:
Other methods for generating exponential variates are discussed by Knuth^{[5]} and Devroye.^{[6]}
The ziggurat algorithm is a fast method for generating exponential variates.
A fast method for generating a set of readyordered exponential variates without using a sorting routine is also available.^{[6]}
This section includes a list of references, but its sources remain unclear because it has insufficient inline citations. (March 2011) 
Other related distributions:
The exponential distribution occurs naturally when describing the lengths of the interarrival times in a homogeneous Poisson process.
The exponential distribution may be viewed as a continuous counterpart of the geometric distribution, which describes the number of Bernoulli trials necessary for a discrete process to change state. In contrast, the exponential distribution describes the time for a continuous process to change state.
In realworld scenarios, the assumption of a constant rate (or probability per unit time) is rarely satisfied. For example, the rate of incoming phone calls differs according to the time of day. But if we focus on a time interval during which the rate is roughly constant, such as from 2 to 4 p.m. during work days, the exponential distribution can be used as a good approximate model for the time until the next phone call arrives. Similar caveats apply to the following examples which yield approximately exponentially distributed variables:
Exponential variables can also be used to model situations where certain events occur with a constant probability per unit length, such as the distance between mutations on a DNA strand, or between roadkills on a given road.^{[citation needed]}
In queuing theory, the service times of agents in a system (e.g. how long it takes for a bank teller etc. to serve a customer) are often modeled as exponentially distributed variables. (The interarrival of customers for instance in a system is typically modeled by the Poisson distribution in most management science textbooks.) The length of a process that can be thought of as a sequence of several independent tasks is better modeled by a variable following the Erlang distribution (which is the distribution of the sum of several independent exponentially distributed variables).
Reliability theory and reliability engineering also make extensive use of the exponential distribution. Because of the memoryless property of this distribution, it is wellsuited to model the constant hazard rate portion of the bathtub curve used in reliability theory. It is also very convenient because it is so easy to add failure rates in a reliability model. The exponential distribution is however not appropriate to model the overall lifetime of organisms or technical devices, because the "failure rates" here are not constant: more failures occur for very young and for very old systems.
In physics, if you observe a gas at a fixed temperature and pressure in a uniform gravitational field, the heights of the various molecules also follow an approximate exponential distribution, known as the Barometric formula. This is a consequence of the entropy property mentioned below.
In hydrology, the exponential distribution is used to analyze extreme values of such variables as monthly and annual maximum values of daily rainfall and river discharge volumes.^{[8]}
Having observed a sample of n data points from an unknown exponential distribution a common task is to use these samples to make predictions about future data from the same source. A common predictive distribution over future samples is the socalled plugin distribution, formed by plugging a suitable estimate for the rate parameter λ into the exponential density function. A common choice of estimate is the one provided by the principle of maximum likelihood, and using this yields the predictive density over a future sample x_{n+1}, conditioned on the observed samples x = (x_{1}, ..., x_{n}) given by
The Bayesian approach provides a predictive distribution which takes into account the uncertainty of the estimated parameter, although this may depend crucially on the choice of prior.
A predictive distribution free of the issues of choosing priors that arise under the subjective Bayesian approach is
which can be considered as
The accuracy of a predictive distribution may be measured using the distance or divergence between the true exponential distribution with rate parameter, λ_{0}, and the predictive distribution based on the sample x. The Kullback–Leibler divergence is a commonly used, parameterisation free measure of the difference between two distributions. Letting Δ(λ_{0}p) denote the Kullback–Leibler divergence between an exponential with rate parameter λ_{0} and a predictive distribution p it can be shown that
where the expectation is taken with respect to the exponential distribution with rate parameter λ_{0} ∈ (0, ∞), and ψ( · ) is the digamma function. It is clear that the CNML predictive distribution is strictly superior to the maximum likelihood plugin distribution in terms of average Kullback–Leibler divergence for all sample sizes n > 0.
