HOME

TheInfoList



OR:

In
statistics Statistics (from German language, German: ', "description of a State (polity), state, a country") is the discipline that concerns the collection, organization, analysis, interpretation, and presentation of data. In applying statistics to a s ...
, sufficiency is a property of a
statistic A statistic (singular) or sample statistic is any quantity computed from values in a sample which is considered for a statistical purpose. Statistical purposes include estimating a population parameter, describing a sample, or evaluating a hypot ...
computed on a sample dataset in relation to a parametric model of the dataset. A sufficient statistic contains all of the information that the dataset provides about the model parameters. It is closely related to the concepts of an ancillary statistic which contains no information about the model parameters, and of a complete statistic which only contains information about the parameters and no ancillary information. A related concept is that of linear sufficiency, which is weaker than ''sufficiency'' but can be applied in some cases where there is no sufficient statistic, although it is restricted to linear estimators. The
Kolmogorov structure function In 1973, Andrey Kolmogorov proposed a non-probabilistic approach to statistics and model selection. Let each datum be a finite binary string and a model be a finite set of binary strings. Consider model classes consisting of models of given maxim ...
deals with individual finite data; the related notion there is the algorithmic sufficient statistic. The concept is due to Sir Ronald Fisher in 1920. Stephen Stigler noted in 1973 that the concept of sufficiency had fallen out of favor in
descriptive statistics A descriptive statistic (in the count noun sense) is a summary statistic that quantitatively describes or summarizes features from a collection of information, while descriptive statistics (in the mass noun sense) is the process of using and an ...
because of the strong dependence on an assumption of the distributional form (see Pitman–Koopman–Darmois theorem below), but remained very important in theoretical work.


Background

Roughly, given a set \mathbf of independent identically distributed data conditioned on an unknown parameter \theta, a sufficient statistic is a function T(\mathbf) whose value contains all the information needed to compute any estimate of the parameter (e.g. a maximum likelihood estimate). Due to the factorization theorem ( see below), for a sufficient statistic T(\mathbf), the probability density can be written as f_(x;\theta) = h(x) \, g(\theta, T(x)). From this factorization, it can easily be seen that the maximum likelihood estimate of \theta will interact with \mathbf only through T(\mathbf). Typically, the sufficient statistic is a simple function of the data, e.g. the sum of all the data points. More generally, the "unknown parameter" may represent a
vector Vector most often refers to: * Euclidean vector, a quantity with a magnitude and a direction * Disease vector, an agent that carries and transmits an infectious pathogen into another living organism Vector may also refer to: Mathematics a ...
of unknown quantities or may represent everything about the model that is unknown or not fully specified. In such a case, the sufficient statistic may be a set of functions, called a ''jointly sufficient statistic''. Typically, there are as many functions as there are parameters. For example, for a
Gaussian distribution In probability theory and statistics, a normal distribution or Gaussian distribution is a type of continuous probability distribution for a real number, real-valued random variable. The general form of its probability density function is f(x ...
with unknown
mean A mean is a quantity representing the "center" of a collection of numbers and is intermediate to the extreme values of the set of numbers. There are several kinds of means (or "measures of central tendency") in mathematics, especially in statist ...
and
variance In probability theory and statistics, variance is the expected value of the squared deviation from the mean of a random variable. The standard deviation (SD) is obtained as the square root of the variance. Variance is a measure of dispersion ...
, the jointly sufficient statistic, from which maximum likelihood estimates of both parameters can be estimated, consists of two functions, the sum of all data points and the sum of all squared data points (or equivalently, the sample mean and
sample variance In probability theory and statistics, variance is the expected value of the squared deviation from the mean of a random variable. The standard deviation (SD) is obtained as the square root of the variance. Variance is a measure of dispersion, ...
). In other words, the
joint probability distribution A joint or articulation (or articular surface) is the connection made between bones, ossicles, or other hard structures in the body which link an animal's skeletal system into a functional whole.Saladin, Ken. Anatomy & Physiology. 7th ed. McGraw- ...
of the data is conditionally independent of the parameter given the value of the sufficient statistic for the parameter. Both the statistic and the underlying parameter can be vectors.


Mathematical definition

A statistic ''t'' = ''T''(''X'') is sufficient for underlying parameter ''θ'' precisely if the
conditional probability distribution In probability theory and statistics, the conditional probability distribution is a probability distribution that describes the probability of an outcome given the occurrence of a particular event. Given two jointly distributed random variables X ...
of the data ''X'', given the statistic ''t'' = ''T''(''X''), does not depend on the parameter ''θ''. Alternatively, one can say the statistic ''T''(''X'') is sufficient for ''θ'' if, for all prior distributions on ''θ'', the
mutual information In probability theory and information theory, the mutual information (MI) of two random variables is a measure of the mutual Statistical dependence, dependence between the two variables. More specifically, it quantifies the "Information conten ...
between ''θ'' and ''T(X)'' equals the mutual information between ''θ'' and ''X''. In other words, the data processing inequality becomes an equality: :I\bigl(\theta ; T(X)\bigr) = I(\theta ; X)


Example

As an example, the sample mean is sufficient for the (unknown) mean ''μ'' of a
normal distribution In probability theory and statistics, a normal distribution or Gaussian distribution is a type of continuous probability distribution for a real-valued random variable. The general form of its probability density function is f(x) = \frac ...
with known variance. Once the sample mean is known, no further information about ''μ'' can be obtained from the sample itself. On the other hand, for an arbitrary distribution the
median The median of a set of numbers is the value separating the higher half from the lower half of a Sample (statistics), data sample, a statistical population, population, or a probability distribution. For a data set, it may be thought of as the “ ...
is not sufficient for the mean: even if the median of the sample is known, knowing the sample itself would provide further information about the population mean. For example, if the observations that are less than the median are only slightly less, but observations exceeding the median exceed it by a large amount, then this would have a bearing on one's inference about the population mean.


Fisher–Neyman factorization theorem

'' Fisher's factorization theorem'' or ''factorization criterion'' provides a convenient characterization of a sufficient statistic. If the
probability density function In probability theory, a probability density function (PDF), density function, or density of an absolutely continuous random variable, is a Function (mathematics), function whose value at any given sample (or point) in the sample space (the s ...
is ƒ''θ''(''x''), then ''T'' is sufficient for ''θ''
if and only if In logic and related fields such as mathematics and philosophy, "if and only if" (often shortened as "iff") is paraphrased by the biconditional, a logical connective between statements. The biconditional is true in two cases, where either bo ...
nonnegative functions ''g'' and ''h'' can be found such that : f(x;\theta)=h(x) \, g(\theta,T(x)), i.e., the density ƒ can be factored into a product such that one factor, ''h'', does not depend on ''θ'' and the other factor, which does depend on ''θ'', depends on ''x'' only through ''T''(''x''). A general proof of this was given by Halmos and Savage and the theorem is sometimes referred to as the Halmos–Savage factorization theorem. The proofs below handle special cases, but an alternative general proof along the same lines can be given. In many simple cases the probability density function is fully specified by \theta and T(x), and h(x)=1 (see
Examples Example may refer to: * ''exempli gratia'' (e.g.), usually read out in English as "for example" * .example, reserved as a domain name that may not be installed as a top-level domain of the Internet ** example.com, example.net, example.org, a ...
). It is easy to see that if ''F''(''t'') is a one-to-one function and ''T'' is a sufficient statistic, then ''F''(''T'') is a sufficient statistic. In particular we can multiply a sufficient statistic by a nonzero constant and get another sufficient statistic.


Likelihood principle interpretation

An implication of the theorem is that when using likelihood-based inference, two sets of data yielding the same value for the sufficient statistic ''T''(''X'') will always yield the same inferences about ''θ''. By the factorization criterion, the likelihood's dependence on ''θ'' is only in conjunction with ''T''(''X''). As this is the same in both cases, the dependence on ''θ'' will be the same as well, leading to identical inferences.


Proof

Due to Hogg and Craig. Let X_1, X_2, \ldots, X_n, denote a random sample from a distribution having the
pdf Portable document format (PDF), standardized as ISO 32000, is a file format developed by Adobe Inc., Adobe in 1992 to present documents, including text formatting and images, in a manner independent of application software, computer hardware, ...
''f''(''x'', ''θ'') for ''ι'' < ''θ'' < ''δ''. Let ''Y''1 = ''u''1(''X''1, ''X''2, ..., ''X''''n'') be a statistic whose pdf is ''g''1(''y''1; ''θ''). What we want to prove is that ''Y''1 = ''u''1(''X''1, ''X''2, ..., ''X''''n'') is a sufficient statistic for ''θ'' if and only if, for some function ''H'', : \prod_^n f(x_i; \theta) = g_1 \left _1 (x_1, x_2, \dots, x_n); \theta \rightH(x_1, x_2, \dots, x_n). First, suppose that : \prod_^n f(x_i; \theta) = g_1 \left _1 (x_1, x_2, \dots, x_n); \theta \rightH(x_1, x_2, \dots, x_n). We shall make the transformation ''y''''i'' = ''u''i(''x''1, ''x''2, ..., ''x''''n''), for ''i'' = 1, ..., ''n'', having inverse functions ''x''''i'' = ''w''''i''(''y''1, ''y''2, ..., ''y''''n''), for ''i'' = 1, ..., ''n'', and Jacobian J = \left _i/y_j \right. Thus, : \prod_^n f \left w_i(y_1, y_2, \dots, y_n); \theta \right = , J, g_1 (y_1; \theta) H \left w_1(y_1, y_2, \dots, y_n), \dots, w_n(y_1, y_2, \dots, y_n) \right The left-hand member is the joint pdf ''g''(''y''1, ''y''2, ..., ''y''''n''; θ) of ''Y''1 = ''u''1(''X''1, ..., ''X''''n''), ..., ''Y''''n'' = ''u''''n''(''X''1, ..., ''X''''n''). In the right-hand member, g_1(y_1;\theta) is the pdf of Y_1, so that H w_1, \dots , w_n, J, is the quotient of g(y_1,\dots,y_n;\theta) and g_1(y_1;\theta); that is, it is the conditional pdf h(y_2, \dots, y_n \mid y_1; \theta) of Y_2,\dots,Y_n given Y_1=y_1. But H(x_1,x_2,\dots,x_n), and thus H\left _1(y_1,\dots,y_n), \dots, w_n(y_1, \dots, y_n))\right/math>, was given not to depend upon \theta. Since \theta was not introduced in the transformation and accordingly not in the Jacobian J, it follows that h(y_2, \dots, y_n \mid y_1; \theta) does not depend upon \theta and that Y_1 is a sufficient statistics for \theta. The converse is proven by taking: :g(y_1,\dots,y_n;\theta)=g_1(y_1; \theta) h(y_2, \dots, y_n \mid y_1), where h(y_2, \dots, y_n \mid y_1) does not depend upon \theta because Y_2 ... Y_n depend only upon X_1 ... X_n, which are independent on \Theta when conditioned by Y_1, a sufficient statistics by hypothesis. Now divide both members by the absolute value of the non-vanishing Jacobian J, and replace y_1, \dots, y_n by the functions u_1(x_1, \dots, x_n), \dots, u_n(x_1,\dots, x_n) in x_1,\dots, x_n. This yields :\frac=g_1\left _1(x_1,\dots,x_n); \theta\right\frac where J^* is the Jacobian with y_1,\dots,y_n replaced by their value in terms x_1, \dots, x_n. The left-hand member is necessarily the joint pdf f(x_1;\theta)\cdots f(x_n;\theta) of X_1,\dots,X_n. Since h(y_2,\dots,y_n\mid y_1), and thus h(u_2,\dots,u_n\mid u_1), does not depend upon \theta, then :H(x_1,\dots,x_n)=\frac is a function that does not depend upon \theta.


Another proof

A simpler more illustrative proof is as follows, although it applies only in the discrete case. We use the shorthand notation to denote the joint probability density of (X, T(X)) by f_\theta(x,t). Since T is a deterministic function of X, we have f_\theta(x,t) = f_\theta(x), as long as t = T(x) and zero otherwise. Therefore: : \begin f_\theta(x) & = f_\theta(x,t) \\ pt& = f_\theta (x\mid t) f_\theta(t) \\ pt& = f(x\mid t) f_\theta(t) \end with the last equality being true by the definition of sufficient statistics. Thus f_\theta(x)=a(x) b_\theta(t) with a(x) = f_(x) and b_\theta(t) = f_\theta(t). Conversely, if f_\theta(x)=a(x) b_\theta(t), we have : \begin f_\theta(t) & = \sum _ f_\theta(x, t) \\ pt& = \sum _ f_\theta(x) \\ pt& = \sum _ a(x) b_\theta(t) \\ pt& = \left( \sum _ a(x) \right) b_\theta(t). \end With the first equality by the definition of pdf for multiple variables, the second by the remark above, the third by hypothesis, and the fourth because the summation is not over t. Let f_(x) denote the conditional probability density of X given T(X). Then we can derive an explicit expression for this: : \begin f_(x) & = \frac \\ pt& = \frac \\ pt& = \frac \\ pt& = \frac. \end With the first equality by definition of conditional probability density, the second by the remark above, the third by the equality proven above, and the fourth by simplification. This expression does not depend on \theta and thus T is a sufficient statistic.


Minimal sufficiency

A sufficient statistic is minimal sufficient if it can be represented as a function of any other sufficient statistic. In other words, ''S''(''X'') is minimal sufficient if and only if #''S''(''X'') is sufficient, and #if ''T''(''X'') is sufficient, then there exists a function ''f'' such that ''S''(''X'') = ''f''(''T''(''X'')). Intuitively, a minimal sufficient statistic ''most efficiently'' captures all possible information about the parameter ''θ''. A useful characterization of minimal sufficiency is that when the density ''f''''θ'' exists, ''S''(''X'') is minimal sufficient if and only if :\frac is independent of ''θ'' :\Longleftrightarrow ''S''(''x'') = ''S''(''y'') This follows as a consequence from Fisher's factorization theorem stated above. A case in which there is no minimal sufficient statistic was shown by Bahadur, 1954. However, under mild conditions, a minimal sufficient statistic does always exist. In particular, in Euclidean space, these conditions always hold if the random variables (associated with P_\theta ) are all discrete or are all continuous. If there exists a minimal sufficient statistic, and this is usually the case, then every complete sufficient statistic is necessarily minimal sufficient (note that this statement does not exclude a pathological case in which a complete sufficient exists while there is no minimal sufficient statistic). While it is hard to find cases in which a minimal sufficient statistic does not exist, it is not so hard to find cases in which there is no complete statistic. The collection of likelihood ratios \left\ for i = 1, ..., k, is a minimal sufficient statistic if the parameter space is discrete \left\.


Examples


Bernoulli distribution

If ''X''1, ...., ''X''''n'' are independent Bernoulli-distributed random variables with expected value ''p'', then the sum ''T''(''X'') = ''X''1 + ... + ''X''''n'' is a sufficient statistic for ''p'' (here 'success' corresponds to ''X''''i'' = 1 and 'failure' to ''X''''i'' = 0; so ''T'' is the total number of successes) This is seen by considering the joint probability distribution: : \Pr\=\Pr\. Because the observations are independent, this can be written as : p^(1-p)^ p^(1-p)^\cdots p^(1-p)^ and, collecting powers of ''p'' and 1 − ''p'', gives : p^(1-p)^=p^(1-p)^ which satisfies the factorization criterion, with ''h''(''x'') = 1 being just a constant. Note the crucial feature: the unknown parameter ''p'' interacts with the data ''x'' only via the statistic ''T''(''x'') = Σ ''x''''i''. As a concrete application, this gives a procedure for distinguishing a fair coin from a biased coin.


Uniform distribution

If ''X''1, ...., ''X''''n'' are independent and uniformly distributed on the interval ,''θ'' then ''T''(''X'') = max(''X''1, ..., ''X''''n'') is sufficient for θ — the sample maximum is a sufficient statistic for the population maximum. To see this, consider the joint
probability density function In probability theory, a probability density function (PDF), density function, or density of an absolutely continuous random variable, is a Function (mathematics), function whose value at any given sample (or point) in the sample space (the s ...
of ''X''  (''X''1,...,''X''''n''). Because the observations are independent, the pdf can be written as a product of individual densities :\begin f_(x_1,\ldots,x_n) &= \frac\mathbf_ \cdots \frac\mathbf_ \\ pt &= \frac \mathbf_\mathbf_ \end where 1 is the
indicator function In mathematics, an indicator function or a characteristic function of a subset of a set is a function that maps elements of the subset to one, and all other elements to zero. That is, if is a subset of some set , then the indicator functio ...
. Thus the density takes form required by the Fisher–Neyman factorization theorem, where ''h''(''x'') = 1, and the rest of the expression is a function of only ''θ'' and ''T''(''x'') = max. In fact, the minimum-variance unbiased estimator (MVUE) for ''θ'' is : \fracT(X). This is the sample maximum, scaled to correct for the
bias Bias is a disproportionate weight ''in favor of'' or ''against'' an idea or thing, usually in a way that is inaccurate, closed-minded, prejudicial, or unfair. Biases can be innate or learned. People may develop biases for or against an individ ...
, and is MVUE by the Lehmann–Scheffé theorem. Unscaled sample maximum ''T''(''X'') is the maximum likelihood estimator for ''θ''.


Uniform distribution (with two parameters)

If X_1,...,X_n are independent and uniformly distributed on the interval alpha, \beta/math> (where \alpha and \beta are unknown parameters), then T(X_1^n)=\left(\min_X_i,\max_X_i\right) is a two-dimensional sufficient statistic for (\alpha\, , \, \beta). To see this, consider the joint
probability density function In probability theory, a probability density function (PDF), density function, or density of an absolutely continuous random variable, is a Function (mathematics), function whose value at any given sample (or point) in the sample space (the s ...
of X_1^n=(X_1,\ldots,X_n). Because the observations are independent, the pdf can be written as a product of individual densities, i.e. :\begin f_(x_1^n) &= \prod_^n \left(\right) \mathbf_ = \left(\right)^n \mathbf_ \\ &= \left(\right)^n \mathbf_ \mathbf_. \end The joint density of the sample takes the form required by the Fisher–Neyman factorization theorem, by letting :\begin h(x_1^n)= 1, \quad g_(x_1^n)= \left(\right)^n \mathbf_ \mathbf_. \end Since h(x_1^n) does not depend on the parameter (\alpha, \beta) and g_(x_1^n) depends only on x_1^n through the function T(X_1^n)= \left(\min_X_i,\max_X_i\right), the Fisher–Neyman factorization theorem implies T(X_1^n) = \left(\min_X_i,\max_X_i\right) is a sufficient statistic for (\alpha\, , \, \beta).


Poisson distribution

If ''X''1, ...., ''X''''n'' are independent and have a
Poisson distribution In probability theory and statistics, the Poisson distribution () is a discrete probability distribution that expresses the probability of a given number of events occurring in a fixed interval of time if these events occur with a known const ...
with parameter ''λ'', then the sum ''T''(''X'') = ''X''1 + ... + ''X''''n'' is a sufficient statistic for ''λ''. To see this, consider the joint probability distribution: : \Pr(X=x)=P(X_1=x_1,X_2=x_2,\ldots,X_n=x_n). Because the observations are independent, this can be written as : \cdot \cdots which may be written as : e^ \lambda^ \cdot which shows that the factorization criterion is satisfied, where ''h''(''x'') is the reciprocal of the product of the factorials. Note the parameter λ interacts with the data only through its sum ''T''(''X'').


Normal distribution

If X_1,\ldots,X_n are independent and normally distributed with expected value \theta (a parameter) and known finite variance \sigma^2, then :T(X_1^n)=\overline=\frac1n\sum_^nX_i is a sufficient statistic for \theta. To see this, consider the joint
probability density function In probability theory, a probability density function (PDF), density function, or density of an absolutely continuous random variable, is a Function (mathematics), function whose value at any given sample (or point) in the sample space (the s ...
of X_1^n=(X_1,\dots,X_n). Because the observations are independent, the pdf can be written as a product of individual densities, i.e. :\begin f_(x_1^n) & = \prod_^n \frac \exp \left (-\frac \right ) \\ pt &= (2\pi\sigma^2)^ \exp \left ( -\sum_^n \frac \right ) \\ pt & = (2\pi\sigma^2)^ \exp \left (-\sum_^n \frac \right ) \\ pt & = (2\pi\sigma^2)^ \exp \left( - \left(\sum_^n(x_i-\overline)^2 + \sum_^n(\theta-\overline)^2 -2\sum_^n(x_i-\overline)(\theta-\overline)\right) \right) \\ pt &= (2\pi\sigma^2)^ \exp \left( - \left (\sum_^n(x_i-\overline)^2 + n(\theta-\overline)^2 \right ) \right ) && \sum_^n(x_i-\overline)(\theta-\overline)=0 \\ pt &= (2\pi\sigma^2)^ \exp \left( - \sum_^n (x_i-\overline)^2 \right ) \exp \left (-\frac (\theta-\overline)^2 \right ) \end The joint density of the sample takes the form required by the Fisher–Neyman factorization theorem, by letting :\begin h(x_1^n) &= (2\pi\sigma^2)^ \exp \left( - \sum_^n (x_i-\overline)^2 \right ) \\ ptg_\theta(x_1^n) &= \exp \left (-\frac (\theta-\overline)^2 \right ) \end Since h(x_1^n) does not depend on the parameter \theta and g_(x_1^n) depends only on x_1^n through the function :T(X_1^n)=\overline=\frac1n\sum_^nX_i, the Fisher–Neyman factorization theorem implies T(X_1^n) is a sufficient statistic for \theta. If \sigma^2 is unknown and since s^2 = \frac \sum_^n \left(x_i - \overline \right)^2 , the above likelihood can be rewritten as :\begin f_(x_1^n)= (2\pi\sigma^2)^ \exp \left( -\fracs^2 \right) \exp \left (-\frac (\theta-\overline)^2 \right ) . \end The Fisher–Neyman factorization theorem still holds and implies that (\overline,s^2) is a joint sufficient statistic for ( \theta , \sigma^2) .


Exponential distribution

If X_1,\dots,X_n are independent and
exponentially distributed In probability theory and statistics, the exponential distribution or negative exponential distribution is the probability distribution of the distance between events in a Poisson point process, i.e., a process in which events occur continuous ...
with expected value ''θ'' (an unknown real-valued positive parameter), then T(X_1^n)=\sum_^nX_i is a sufficient statistic for θ. To see this, consider the joint
probability density function In probability theory, a probability density function (PDF), density function, or density of an absolutely continuous random variable, is a Function (mathematics), function whose value at any given sample (or point) in the sample space (the s ...
of X_1^n=(X_1,\dots,X_n). Because the observations are independent, the pdf can be written as a product of individual densities, i.e. :\begin f_(x_1^n) &= \prod_^n \, e^ = \, e^. \end The joint density of the sample takes the form required by the Fisher–Neyman factorization theorem, by letting :\begin h(x_1^n)= 1,\,\,\, g_(x_1^n)= \, e^. \end Since h(x_1^n) does not depend on the parameter \theta and g_(x_1^n) depends only on x_1^n through the function T(X_1^n)=\sum_^nX_i the Fisher–Neyman factorization theorem implies T(X_1^n)=\sum_^nX_i is a sufficient statistic for \theta.


Gamma distribution

If X_1,\dots,X_n are independent and distributed as a \Gamma(\alpha \, , \, \beta) , where \alpha and \beta are unknown parameters of a Gamma distribution, then T(X_1^n) = \left( \prod_^n , \sum_^n X_i \right) is a two-dimensional sufficient statistic for (\alpha, \beta). To see this, consider the joint
probability density function In probability theory, a probability density function (PDF), density function, or density of an absolutely continuous random variable, is a Function (mathematics), function whose value at any given sample (or point) in the sample space (the s ...
of X_1^n=(X_1,\dots,X_n). Because the observations are independent, the pdf can be written as a product of individual densities, i.e. :\begin f_(x_1^n) &= \prod_^n \left(\right) x_i^ e^ \\ pt &= \left(\right)^n \left(\prod_^n x_i\right)^ e^. \end The joint density of the sample takes the form required by the Fisher–Neyman factorization theorem, by letting :\begin h(x_1^n)= 1,\,\,\, g_(x_1^n)= \left(\right)^n \left(\prod_^n x_i\right)^ e^. \end Since h(x_1^n) does not depend on the parameter (\alpha\, , \, \beta) and g_(x_1^n) depends only on x_1^n through the function T(x_1^n)= \left( \prod_^n x_i, \sum_^n x_i \right), the Fisher–Neyman factorization theorem implies T(X_1^n)= \left( \prod_^n X_i, \sum_^n X_i \right) is a sufficient statistic for (\alpha\, , \, \beta).


Rao–Blackwell theorem

Sufficiency finds a useful application in the Rao–Blackwell theorem, which states that if ''g''(''X'') is any kind of estimator of ''θ'', then typically the conditional expectation of ''g''(''X'') given sufficient statistic ''T''(''X'') is a better (in the sense of having lower
variance In probability theory and statistics, variance is the expected value of the squared deviation from the mean of a random variable. The standard deviation (SD) is obtained as the square root of the variance. Variance is a measure of dispersion ...
) estimator of ''θ'', and is never worse. Sometimes one can very easily construct a very crude estimator ''g''(''X''), and then evaluate that conditional expected value to get an estimator that is in various senses optimal.


Exponential family

According to the Pitman–Koopman–Darmois theorem, among families of probability distributions whose domain does not vary with the parameter being estimated, only in exponential families is there a sufficient statistic whose dimension remains bounded as sample size increases. Intuitively, this states that nonexponential families of distributions on the real line require
nonparametric statistics Nonparametric statistics is a type of statistical analysis that makes minimal assumptions about the underlying distribution of the data being studied. Often these models are infinite-dimensional, rather than finite dimensional, as in parametric s ...
to fully capture the information in the data. Less tersely, suppose X_n, n = 1, 2, 3, \dots are independent identically distributed real random variables whose distribution is known to be in some family of probability distributions, parametrized by \theta, satisfying certain technical regularity conditions, then that family is an ''exponential'' family if and only if there is a \R^m-valued sufficient statistic T(X_1, \dots, X_n) whose number of scalar components m does not increase as the sample size ''n'' increases. This theorem shows that the existence of a finite-dimensional, real-vector-valued sufficient statistics sharply restricts the possible forms of a family of distributions on the real line. When the parameters or the random variables are no longer real-valued, the situation is more complex.


Other types of sufficiency


Bayesian sufficiency

An alternative formulation of the condition that a statistic be sufficient, set in a Bayesian context, involves the posterior distributions obtained by using the full data-set and by using only a statistic. Thus the requirement is that, for almost every ''x'', :\Pr(\theta\mid X=x) = \Pr(\theta\mid T(X)=t(x)). More generally, without assuming a parametric model, we can say that the statistics ''T'' is ''predictive sufficient'' if :\Pr(X'=x'\mid X=x) = \Pr(X'=x'\mid T(X)=t(x)). It turns out that this "Bayesian sufficiency" is a consequence of the formulation above, however they are not directly equivalent in the infinite-dimensional case. A range of theoretical results for sufficiency in a Bayesian context is available.


Linear sufficiency

A concept called "linear sufficiency" can be formulated in a Bayesian context, and more generally. First define the best linear predictor of a vector ''Y'' based on ''X'' as \hat E \mid X/math>. Then a linear statistic ''T''(''x'') is linear sufficient if :\hat E theta\mid X \hat E theta\mid T(X).


See also

* Completeness of a statistic * Basu's theorem on independence of complete sufficient and ancillary statistics * Lehmann–Scheffé theorem: a complete sufficient estimator is the best estimator of its expectation * Rao–Blackwell theorem * Chentsov's theorem * Sufficient dimension reduction * Ancillary statistic


Notes


References

* * *Dodge, Y. (2003) ''The Oxford Dictionary of Statistical Terms'', OUP. {{DEFAULTSORT:Sufficient Statistic Statistical theory Statistical principles Articles containing proofs factorization