Probability distribution


In probability theory and statistics, a probability distribution is the mathematical function that gives the probabilities of occurrence of different possible outcomes for an experiment.[1][2] It is a mathematical description of a random phenomenon in terms of its sample space and the probabilities of events (subsets of the sample space).[3]

For instance, if X is used to denote the outcome of a coin toss ("the experiment"), then the probability distribution of X would take the value 0.5 (1 in 2 or 1/2) for X = heads, and 0.5 for X = tails (assuming that the coin is fair). Examples of random phenomena include the weather conditions at some future date, the height of a randomly selected person, the fraction of male students in a school, the results of a survey to be conducted, etc.[4]


The probability mass function (pmf)   specifies the probability distribution for the sum   of counts from two dice. For example, the figure shows that  . The pmf allows the computation of probabilities of events such as  , and all other probabilities in the distribution.

A probability distribution is a mathematical description of the probabilities of events, subsets of the sample space. The sample space, often denoted by  , is the set of all possible outcomes of a random phenomenon being observed; it may be any set: a set of real numbers, a set of vectors, a set of arbitrary non-numerical values, etc. For example, the sample space of a coin flip would be Ω = {heads, tails}.

To define probability distributions for the specific case of random variables (so the sample space can be seen as a numeric set), it is common to distinguish between discrete and absolutely continuous random variables. In the discrete case, it is sufficient to specify a probability mass function   assigning a probability to each possible outcome: for example, when throwing a fair dice, each of the six values 1 to 6 has the probability 1/6. The probability of an event is then defined to be the sum of the probabilities of the outcomes that satisfy the event; for example, the probability of the event "the die rolls an even value" is


In contrast, when a random variable takes values from a continuum then typically, any individual outcome has probability zero and only events that include infinitely many outcomes, such as intervals, can have positive probability. For example, consider measuring the weight of a piece of ham in the supermarket, and assume the scale has many digits of precision. The probability that it weighs exactly 500 g is zero, as it will most likely have some non-zero decimal digits. Nevertheless, one might demand, in quality control, that a package of "500 g" of ham must weigh between 490 g and 510 g with at least 98% probability, and this demand is less sensitive to the accuracy of measurement instruments.

The left shows the probability density function. The right shows the cumulative distribution function, for which the value at a equals the area under the probability density curve to the left of a.

Absolutely continuous probability distributions can be described in several ways. The probability density function describes the infinitesimal probability of any given value, and the probability that the outcome lies in a given interval can be computed by integrating the probability density function over that interval.[5] An alternative description of the distribution is by means of the cumulative distribution function, which describes the probability that the random variable is no larger than a given value (i.e.,   for some  ). The cumulative distribution function is the area under the probability density function from   to  , as described by the picture to the right.[6]

General probability definitionEdit

A probability distribution can be described in various forms, such as by a probability mass function or a cumulative distribution function. One of the most general descriptions, which applies for absolutely continuous and discrete variables, is by means of a probability function   whose input space   is related[clarification needed] to the sample space, and gives a real number probability as its output.[citation needed]

The probability function   can take as argument subsets of the sample space itself, as in the coin toss example, where the function   was defined so that P(heads) = 0.5 and P(tails) = 0.5. However, because of the widespread use of random variables, which transform the sample space into a set of numbers (e.g.,  ,  ), it is more common to study probability distributions whose argument are subsets of these particular kinds of sets (number sets),[7] and all probability distributions discussed in this article are of this type. It is common to denote as   the probability that a certain value of the variable   belongs to a certain event  .[4][8]

The above probability function only characterizes a probability distribution if it satisfies all the Kolmogorov axioms, that is:

  1.  , so the probability is non-negative
  2.  , so no probability exceeds  
  3.   for any disjoint family of sets  

The concept of probability function is made more rigorous by defining it as the element of a probability space  , where   is the set of possible outcomes,   is the set of all subsets   whose probability can be measured, and   is the probability function, or probability measure, that assigns a probability to each of these measurable subsets  .[9]

Probability distributions usually belong to one of two classes. A discrete probability distribution is applicable to the scenarios where the set of possible outcomes is discrete (e.g. a coin toss, a roll of a die) and the probabilities are encoded by a discrete list of the probabilities of the outcomes; in this case the discrete probability distribution is known as probability mass function. On the other hand, absolutely continuous probability distributions are applicable to scenarios where the set of possible outcomes can take on values in a continuous range (e.g. real numbers), such as the temperature on a given day. In the absolutely continuous case, probabilities are described by a probability density function, and the probability distribution is by definition the integral of the probability density function.[4][5][8] The normal distribution is a commonly encountered absolutely continuous probability distribution. More complex experiments, such as those involving stochastic processes defined in continuous time, may demand the use of more general probability measures.

A probability distribution whose sample space is one-dimensional (for example real numbers, list of labels, ordered labels or binary) is called univariate, while a distribution whose sample space is a vector space of dimension 2 or more is called multivariate. A univariate distribution gives the probabilities of a single random variable taking on various different values; a multivariate distribution (a joint probability distribution) gives the probabilities of a random vector – a list of two or more random variables – taking on various combinations of values. Important and commonly encountered univariate probability distributions include the binomial distribution, the hypergeometric distribution, and the normal distribution. A commonly encountered multivariate distribution is the multivariate normal distribution.

Besides the probability function, the cumulative distribution function, the probability mass function and the probability density function, the moment generating function and the characteristic function also serve to identify a probability distribution, as they uniquely determine an underlying cumulative distribution function.[10]

The probability density function (pdf) of the normal distribution, also called Gaussian or "bell curve", the most important absolutely continuous random distribution. As notated on the figure, the probabilities of intervals of values correspond to the area under the curve.


Some key concepts and terms, widely used in the literature on the topic of probability distributions, are listed below.[1]

Basic termsEdit

  • Random variable: takes values from a sample space; probabilities describe which values and set of values are taken more likely.
  • Event: set of possible values (outcomes) of a random variable that occurs with a certain probability.
  • Probability function or probability measure: describes the probability   that the event   occurs.[11]
  • Cumulative distribution function: function evaluating the probability that   will take a value less than or equal to   for a random variable (only for real-valued random variables).
  • Quantile function: the inverse of the cumulative distribution function. Gives   such that, with probability  ,   will not exceed  .

Discrete probability distributionsEdit

Absolutely continuous probability distributionsEdit

  • Absolutely continuous probability distribution: for many random variables with uncountably many values.
  • Probability density function (pdf) or probability density: function whose value at any given sample (or point) in the sample space (the set of possible values taken by the random variable) can be interpreted as providing a relative likelihood that the value of the random variable would equal that sample.

Related termsEdit

  • Support: set of values that can be assumed with non-zero probability by the random variable. For a random variable  , it is sometimes denoted as  .
  • Tail:[12] the regions close to the bounds of the random variable, if the pmf or pdf are relatively low therein. Usually has the form  ,   or a union thereof.
  • Head:[12] the region where the pmf or pdf is relatively high. Usually has the form  .
  • Expected value or mean: the weighted average of the possible values, using their probabilities as their weights; or the continuous analog thereof.
  • Median: the value such that the set of values less than the median, and the set greater than the median, each have probabilities no greater than one-half.
  • Mode: for a discrete random variable, the value with highest probability; for an absolutely continuous random variable, a location at which the probability density function has a local peak.
  • Quantile: the q-quantile is the value   such that  .
  • Variance: the second moment of the pmf or pdf about the mean; an important measure of the dispersion of the distribution.
  • Standard deviation: the square root of the variance, and hence another measure of dispersion.
  • Symmetry: a property of some distributions in which the portion of the distribution to the left of a specific value (usually the median) is a mirror image of the portion to its right.
  • Skewness: a measure of the extent to which a pmf or pdf "leans" to one side of its mean. The third standardized moment of the distribution.
  • Kurtosis: a measure of the "fatness" of the tails of a pmf or pdf. The fourth standardized moment of the distribution.

Cumulative distribution functionEdit

In the special case of a real-valued random variable, the probability distribution can equivalently be represented by a cumulative distribution function instead of a probability measure. The cumulative distribution function of a random variable   with regard to a probability distribution   is defined as


The cumulative distribution function of any real-valued random variable has the properties:

  •   is non-decreasing;
  •   is right-continuous;
  •  ;
  •   and  ; and
  •  .

Conversely, any function   that satisfies the first four of the properties above is the cumulative distribution function of some probability distribution on the real numbers.[13]

Any probability distribution can be decomposed as the sum of a discrete, an absolutely continuous and a singular continuous distribution,[14] and thus any cumulative distribution function admits a decomposition as the sum of the three according cumulative distribution functions.

Discrete probability distributionEdit

The probability mass function of a discrete probability distribution. The probabilities of the singletons {1}, {3}, and {7} are respectively 0.2, 0.5, 0.3. A set not containing any of these points has probability zero.
The cdf of a discrete probability distribution, ...
... of a continuous probability distribution, ...
... of a distribution which has both a continuous part and a discrete part.

A discrete probability distribution is the probability distribution of a random variable that can take on only a countable number of values[15] (almost surely)[16] which means that the probability of any event   can be expressed as a (finite or countably infinite) sum:

where   is a countable set. Thus the discrete random variables are exactly those with a probability mass function  . In the case where the range of values is countably infinite, these values have to decline to zero fast enough for the probabilities to add up to 1. For example, if   for  , the sum of probabilities would be  .

A discrete random variable is a random variable whose probability distribution is discrete.

Well-known discrete probability distributions used in statistical modeling include the Poisson distribution, the Bernoulli distribution, the binomial distribution, the geometric distribution, the negative binomial distribution and categorical distribution.[3] When a sample (a set of observations) is drawn from a larger population, the sample points have an empirical distribution that is discrete, and which provides information about the population distribution. Additionally, the discrete uniform distribution is commonly used in computer programs that make equal-probability random selections between a number of choices.

Cumulative distribution functionEdit

A real-valued discrete random variable can equivalently be defined as a random variable whose cumulative distribution function increases only by jump discontinuities—that is, its cdf increases only where it "jumps" to a higher value, and is constant in intervals without jumps. The points where jumps occur are precisely the values which the random variable may take. Thus the cumulative distribution function has the form


Note that the points where the cdf jumps always form a countable set; this may be any countable set and thus may even be dense in the real numbers.

Dirac delta representationEdit

A discrete probability distribution is often represented with Dirac measures, the probability distributions of deterministic random variables. For any outcome  , let   be the Dirac measure concentrated at  . Given a discrete probability distribution, there is a countable set   with   and a probability mass function  . If   is any event, then

or in short,

Similarly, discrete distributions can be represented with the Dirac delta function as a generalized probability density function  , where

which means
for any event  [17]

Indicator-function representationEdit

For a discrete random variable  , let   be the values it can take with non-zero probability. Denote


These are disjoint sets, and for such sets


It follows that the probability that   takes any value except for   is zero, and thus one can write   as


except on a set of probability zero, where   is the indicator function of  . This may serve as an alternative definition of discrete random variables.

One-point distributionEdit

A special case is the discrete distribution of a random variable that can take on only one fixed value; in other words, it is a deterministic distribution. Expressed formally, the random variable   has a one-point distribution if it has a possible outcome   such that  [18] All other possible outcomes then have probability 0. Its cumulative distribution function jumps immediately from 0 to 1.

Absolutely continuous probability distributionEdit

An absolutely continuous probability distribution is a probability distribution on the real numbers with uncountably many possible values, such as a whole interval in the real line, and where the probability of any event can be expressed as an integral.[19] More precisely, a real random variable   has an absolutely continuous probability distribution if there is a function   such that for each interval   the probability of   belonging to   is given by the integral of   over  :[20][21]

This is the definition of a probability density function, so that absolutely continuous probability distributions are exactly those with a probability density function. In particular, the probability for   to take any single value   (that is,  ) is zero, because an integral with coinciding upper and lower limits is always equal to zero. If the interval   is replaced by any measurable set  , the according equality still holds:

An absolutely continuous random variable is a random variable whose probability distribution is absolutely continuous.

There are many examples of absolutely continuous probability distributions: normal, uniform, chi-squared, and others.

Cumulative distribution functionEdit

Absolutely continuous probability distributions as defined above are precisely those with an absolutely continuous cumulative distribution function. In this case, the cumulative distribution function   has the form

where   is a density of the random variable   with regard to the distribution  .

Note on terminology: Absolutely continuous distributions ought to be distinguished from continuous distributions, which are those having a continuous cumulative distribution function. Every absolutely continuous distribution is a continuous distribution but the converse is not true, there exist singular distributions, which are neither absolutely continuous nor discrete nor a mixture of those, and do not have a density. An example is given by the Cantor distribution. Some authors however use the term "continuous distribution" to denote all distributions whose cumulative distribution function is absolutely continuous, i.e. refer to absolutely continuous distributions as continuous distributions.[4]

For a more general definition of density functions and the equivalent absolutely continuous measures see absolutely continuous measure.

Kolmogorov definitionEdit

In the measure-theoretic formalization of probability theory, a random variable is defined as a measurable function   from a probability space   to a measurable space  . Given that probabilities of events of the form   satisfy Kolmogorov's probability axioms, the probability distribution of   is the image measure   of   , which is a probability measure on   satisfying  .[22][23][24]

Other kinds of distributionsEdit

One solution for the Rabinovich–Fabrikant equations. What is the probability of observing a state on a certain place of the support (i.e., the red subset)?

Absolutely continuous and discrete distributions with support on   or   are extremely useful to model a myriad of phenomena,[4][6] since most practical distributions are supported on relatively simple subsets, such as hypercubes or balls. However, this is not always the case, and there exist phenomena with supports that are actually complicated curves   within some space   or similar. In these cases, the probability distribution is supported on the image of such curve, and is likely to be determined empirically, rather than finding a closed formula for it.[25]

One example is shown in the figure to the right, which displays the evolution of a system of differential equations (commonly known as the Rabinovich–Fabrikant equations) that can be used to model the behaviour of Langmuir waves in plasma.[26] When this phenomenon is studied, the observed states from the subset are as indicated in red. So one could ask what is the probability of observing a state in a certain position of the red subset; if such a probability exists, it is called the probability measure of the system.[27][25]

This kind of complicated support appears quite frequently in dynamical systems. It is not simple to establish that the system has a probability measure, and the main problem is the following. Let   be instants in time and   a subset of the support; if the probability measure exists for the system, one would expect the frequency of observing states inside set   would be equal in interval   and  , which might not happen; for example, it could oscillate similar to a sine,  , whose limit when   does not converge. Formally, the measure exists only if the limit of the relative frequency converges when the system is observed into the infinite future.[28] The branch of dynamical systems that studies the existence of a probability measure is ergodic theory.

Note that even in these cases, the probability distribution, if it exists, might still be termed "absolutely continuous" or "discrete" depending on whether the support is uncountable or countable, respectively.

Random number generationEdit

Most algorithms are based on a pseudorandom number generator that produces numbers   that are uniformly distributed in the half-open interval [0, 1). These random variates   are then transformed via some algorithm to create a new random variate having the required probability distribution. With this source of uniform pseudo-randomness, realizations of any random variable can be generated.[29]

For example, suppose   has a uniform distribution between 0 and 1. To construct a random Bernoulli variable for some  , we define

so that

This random variable X has a Bernoulli distribution with parameter  .[29] Note that this is a transformation of discrete random variable.

For a distribution function   of an absolutely continuous random variable, an absolutely continuous random variable must be constructed.  , an inverse function of  , relates to the uniform variable  :


For example, suppose a random variable that has an exponential distribution   must be constructed.

so   and if   has a   distribution, then the random variable   is defined by  . This has an exponential distribution of  .[29]

A frequent problem in statistical simulations (the Monte Carlo method) is the generation of pseudo-random numbers that are distributed in a given way.

Common probability distributions and their applicationsEdit

The concept of the probability distribution and the random variables which they describe underlies the mathematical discipline of probability theory, and the science of statistics. There is spread or variability in almost any value that can be measured in a population (e.g. height of people, durability of a metal, sales growth, traffic flow, etc.); almost all measurements are made with some intrinsic error; in physics, many processes are described probabilistically, from the kinetic properties of gases to the quantum mechanical description of fundamental particles. For these and many other reasons, simple numbers are often inadequate for describing a quantity, while probability distributions are often more appropriate.

The following is a list of some of the most common probability distributions, grouped by the type of process that they are related to. For a more complete list, see list of probability distributions, which groups by the nature of the outcome being considered (discrete, absolutely continuous, multivariate, etc.)

All of the univariate distributions below are singly peaked; that is, it is assumed that the values cluster around a single point. In practice, actually observed quantities may cluster around multiple values. Such quantities can be modeled using a mixture distribution.

Linear growth (e.g. errors, offsets)Edit

  • Normal distribution (Gaussian distribution), for a single such quantity; the most commonly used absolutely continuous distribution

Exponential growth (e.g. prices, incomes, populations)Edit

Uniformly distributed quantitiesEdit

Bernoulli trials (yes/no events, with a given probability)Edit

Categorical outcomes (events with K possible outcomes)Edit

Poisson process (events that occur independently with a given rate)Edit

Absolute values of vectors with normally distributed componentsEdit

  • Rayleigh distribution, for the distribution of vector magnitudes with Gaussian distributed orthogonal components. Rayleigh distributions are found in RF signals with Gaussian real and imaginary components.
  • Rice distribution, a generalization of the Rayleigh distributions for where there is a stationary background signal component. Found in Rician fading of radio signals due to multipath propagation and in MR images with noise corruption on non-zero NMR signals.

Normally distributed quantities operated with sum of squaresEdit

As conjugate prior distributions in Bayesian inferenceEdit

Some specialized applications of probability distributionsEdit

  • The cache language models and other statistical language models used in natural language processing to assign probabilities to the occurrence of particular words and word sequences do so by means of probability distributions.
  • In quantum mechanics, the probability density of finding the particle at a given point is proportional to the square of the magnitude of the particle's wavefunction at that point (see Born rule). Therefore, the probability distribution function of the position of a particle is described by  , probability that the particle's position x will be in the interval axb in dimension one, and a similar triple integral in dimension three. This is a key principle of quantum mechanics.[31]
  • Probabilistic load flow in power-flow study explains the uncertainties of input variables as probability distribution and provides the power flow calculation also in term of probability distribution.[32]
  • Prediction of natural phenomena occurrences based on previous frequency distributions such as tropical cyclones, hail, time in between events, etc.[33]


Probability distribution fitting or simply distribution fitting is the fitting of a probability distribution to a series of data concerning the repeated measurement of a variable phenomenon. The aim of distribution fitting is to predict the probability or to forecast the frequency of occurrence of the magnitude of the phenomenon in a certain interval.

There are many probability distributions (see list of probability distributions) of which some can be fitted more closely to the observed frequency of the data than others, depending on the characteristics of the phenomenon and of the distribution. The distribution giving a close fit is supposed to lead to good predictions.

In distribution fitting, therefore, one needs to select a distribution that suits the data well.

See alsoEdit




  1. ^ a b Everitt, Brian (2006). The Cambridge dictionary of statistics (3rd ed.). Cambridge, UK: Cambridge University Press. ISBN 978-0-511-24688-3. OCLC 161828328.
  2. ^ Ash, Robert B. (2008). Basic probability theory (Dover ed.). Mineola, N.Y.: Dover Publications. pp. 66–69. ISBN 978-0-486-46628-6. OCLC 190785258.
  3. ^ a b Evans, Michael; Rosenthal, Jeffrey S. (2010). Probability and statistics: the science of uncertainty (2nd ed.). New York: W.H. Freeman and Co. p. 38. ISBN 978-1-4292-2462-8. OCLC 473463742.
  4. ^ a b c d e Ross, Sheldon M. (2010). A first course in probability. Pearson.
  5. ^ a b " What is a Probability Distribution". Retrieved 2020-09-10.
  6. ^ a b A modern introduction to probability and statistics : understanding why and how. Dekking, Michel, 1946-. London: Springer. 2005. ISBN 978-1-85233-896-1. OCLC 262680588.{{cite book}}: CS1 maint: others (link)
  7. ^ Walpole, R.E.; Myers, R.H.; Myers, S.L.; Ye, K. (1999). Probability and statistics for engineers. Prentice Hall.
  8. ^ a b DeGroot, Morris H.; Schervish, Mark J. (2002). Probability and Statistics. Addison-Wesley.
  9. ^ Billingsley, P. (1986). Probability and measure. Wiley. ISBN 9780471804789.
  10. ^ Shephard, N.G. (1991). "From characteristic function to distribution function: a simple framework for the theory". Econometric Theory. 7 (4): 519–529. doi:10.1017/S0266466600004746. S2CID 14668369.
  11. ^ Chapters 1 and 2 of Vapnik (1998)
  12. ^ a b More information and examples can be found in the articles Heavy-tailed distribution, Long-tailed distribution, fat-tailed distribution
  13. ^ Erhan, Çınlar (2011). Probability and stochastics. New York: Springer. p. 57. ISBN 9780387878584.
  14. ^ see Lebesgue's decomposition theorem
  15. ^ Erhan, Çınlar (2011). Probability and stochastics. New York: Springer. p. 51. ISBN 9780387878591. OCLC 710149819.
  16. ^ Cohn, Donald L. (1993). Measure theory. Birkhäuser.
  17. ^ Khuri, André I. (March 2004). "Applications of Dirac's delta function in statistics". International Journal of Mathematical Education in Science and Technology. 35 (2): 185–195. doi:10.1080/00207390310001638313. ISSN 0020-739X. S2CID 122501973.
  18. ^ Fisz, Marek (1963). Probability Theory and Mathematical Statistics (3rd ed.). John Wiley & Sons. p. 129. ISBN 0-471-26250-1.
  19. ^ Jeffrey Seth Rosenthal (2000). A First Look at Rigorous Probability Theory. World Scientific.
  20. ^ Chapter 3.2 of DeGroot & Schervish (2002)
  21. ^ Bourne, Murray. "11. Probability Distributions - Concepts". Retrieved 2020-09-10.
  22. ^ W., Stroock, Daniel (1999). Probability theory : an analytic view (Rev. ed.). Cambridge [England]: Cambridge University Press. p. 11. ISBN 978-0521663496. OCLC 43953136.
  23. ^ Kolmogorov, Andrey (1950) [1933]. Foundations of the theory of probability. New York, USA: Chelsea Publishing Company. pp. 21–24.
  24. ^ Joyce, David (2014). "Axioms of Probability" (PDF). Clark University. Retrieved December 5, 2019.
  25. ^ a b Alligood, K.T.; Sauer, T.D.; Yorke, J.A. (1996). Chaos: an introduction to dynamical systems. Springer.
  26. ^ Rabinovich, M.I.; Fabrikant, A.L. (1979). "Stochastic self-modulation of waves in nonequilibrium media". J. Exp. Theor. Phys. 77: 617–629. Bibcode:1979JETP...50..311R.
  27. ^ Section 1.9 of Ross, S.M.; Peköz, E.A. (2007). A second course in probability (PDF).
  28. ^ Walters, Peter (2000). An Introduction to Ergodic Theory. Springer.
  29. ^ a b c Dekking, Frederik Michel; Kraaikamp, Cornelis; Lopuhaä, Hendrik Paul; Meester, Ludolf Erwin (2005), "Why probability and statistics?", A Modern Introduction to Probability and Statistics, Springer London, pp. 1–11, doi:10.1007/1-84628-168-7_1, ISBN 978-1-85233-896-1
  30. ^ Bishop, Christopher M. (2006). Pattern recognition and machine learning. New York: Springer. ISBN 0-387-31073-8. OCLC 71008143.
  31. ^ Chang, Raymond. (2014). Physical chemistry for the chemical sciences. Thoman, John W., Jr., 1960-. [Mill Valley, California]. pp. 403–406. ISBN 978-1-68015-835-9. OCLC 927509011.
  32. ^ Chen, P.; Chen, Z.; Bak-Jensen, B. (April 2008). "Probabilistic load flow: A review". 2008 Third International Conference on Electric Utility Deregulation and Restructuring and Power Technologies. pp. 1586–1591. doi:10.1109/drpt.2008.4523658. ISBN 978-7-900714-13-8. S2CID 18669309.
  33. ^ Maity, Rajib (2018-04-30). Statistical methods in hydrology and hydroclimatology. Singapore. ISBN 978-981-10-8779-0. OCLC 1038418263.


  • den Dekker, A. J.; Sijbers, J. (2014). "Data distributions in magnetic resonance images: A review". Physica Medica. 30 (7): 725–741. doi:10.1016/j.ejmp.2014.05.002. PMID 25059432.
  • Vapnik, Vladimir Naumovich (1998). Statistical Learning Theory. John Wiley and Sons.

External linksEdit