Covariance

This article is about the measure of linear relation between random variables. For other uses, see Covariance (disambiguation).

In probability theory and statistics, covariance is a measure of how much two variables change together. Variance is a special case of the covariance when the two variables are identical.

\those of X times those of Y. By contrast, correlation, which depends on the covariance, is a dimensionless measure of linear dependence.

Properties

If X, Y, W, and V are real-valued random variables and a, b, c, d are constant ("constant" in this context means non-random), then the following facts are a consequence of the definition of covariance:

$\operatorname {Cov} (X,a)=0\,$

$\operatorname {Cov} (X,X)=\operatorname {Var} (X)\,$

$\operatorname {Cov} (X,Y)=\operatorname {Cov} (Y,X)\,$

$\operatorname {Cov} (aX,bY)=ab\,\operatorname {Cov} (X,Y)\,$

$\operatorname {Cov} (X+a,Y+b)=\operatorname {Cov} (X,Y)\,$

$\operatorname {Cov} (aX+bY,cW+dV)=ac\,\operatorname {Cov} (X,W)+ad\,\operatorname {Cov} (X,V)+bc\,\operatorname {Cov} (Y,W)+bd\,\operatorname {Cov} (Y,V)\,$

For sequences X₁, ..., X_n and Y₁, ..., Y_m of random variables, we have

$\operatorname {Cov} \left(\sum _{i=1}^{n}{X_{i}},\sum _{j=1}^{m}{Y_{j}}\right)=\sum _{i=1}^{n}{\sum _{j=1}^{m}{\operatorname {Cov} \left(X_{i},Y_{j}\right)}}.\,$

For a sequence X₁, ..., X_n of random variables, and constants a₁, ..., a_n, we have

$\operatorname {Var} \left(\sum _{i=1}^{n}a_{i}X_{i}\right)=\sum _{i=1}^{n}a_{i}^{2}\operatorname {Var} (X_{i})+2\sum _{i,j\,:\,i<j}a_{i}a_{j}\operatorname {Cov} (X_{i},X_{j}).$

Incremental computation

Covariance can be computed efficiently from incrementally available values using a generalization of the computational formula for the variance:

$\operatorname {Cov} (X_{i},X_{j})=\operatorname {E} \left((X_{i}-\operatorname {E} (X_{i}))(X_{j}-\operatorname {E} (X_{j}))\right)=\operatorname {E} (X_{i}X_{j})-\operatorname {E} (X_{i})\operatorname {E} (X_{j})$

Uncorrelatedness and independence

If X and Y are independent, then their covariance is zero. This follows because under independence,

$\operatorname {E} (X\cdot Y)=E(X)\cdot E(Y).$

The converse, however, is generally not true: Some pairs of random variables have covariance zero although they are not independent. Under some additional assumptions, covariance zero sometimes does entail independence, as for example in the case of multivariate normal distributions.

Relationship to inner products

Many of the properties of covariance can be extracted elegantly by observing that it satisfies similar properties to those of an inner product:

1. bilinear: for constants a and b and random variables X, Y, and U, Cov(aX + bY, U) = a Cov(X, U) + b Cov(Y, U)
2. symmetric: Cov(X, Y) = Cov(Y, X)
3. positive semi-definite: Var(X) = Cov(X, X) ≥ 0, and Cov(X, X) = 0 implies that X is a constant random variable (K).

In fact these properties imply that the covariance defines an inner product over the quotient vector space obtained by taking the subspace of random variables with finite second moment and identifying any two that differ by a constant. (This identification turns the positive semi-definiteness above into positive definiteness.) That quotient vector space is isomorphic to the subspace of random variables with finite second moment and mean zero; on that subspace, the covariance is exactly the L² inner product of real-valued functions on the sample space.

Covariance operator, bilinear form, and function

More generally, for a probability measure P on a Hilbert space H with inner product $\langle \cdot ,\cdot \rangle$, the covariance of P is the bilinear form Cov: H × H → R given by

$\mathrm {Cov} (x,y)=\int _{H}\langle x,z\rangle \langle y,z\rangle \,\mathrm {d} \mathbf {P} (z)$

for all x and y in H. The covariance operator C is then defined by

$\mathrm {Cov} (x,y)=\langle Cx,y\rangle$

(from the Riesz representation theorem, such operator exists if Cov is bounded). Since Cov is symmetric in its arguments, the covariance operator is self-adjoint (the infinite-dimensional analogy of the transposition symmetry in the finite-dimensional case). When P is a centred Gaussian measure, C is also a nuclear operator. In particular, it is a compact operator of trace class, that is, it has finite trace.

Even more generally, for a probability measure P on a Banach space B, the covariance of P is the bilinear form on the algebraic dual B^#, defined by

$\mathrm {Cov} (x,y)=\int _{B}\langle x,z\rangle \langle y,z\rangle \,\mathrm {d} \mathbf {P} (z)$

where $\langle x,z\rangle$ is now the value of the linear functional x on the element z.

Quite similarly, the covariance function of a function-valued random element (in special cases called random process or random field) z is

$\mathrm {Cov} (x,y)=\int z(x)z(y)\,\mathrm {d} \mathbf {P} (z)=E(z(x)z(y)),$

where z(x) is now the value of the function z at the point x, i.e., the value of the linear functional $u\mapsto u(x)$ evaluated at z.

Comments

The covariance is sometimes called a measure of "linear dependence" between the two random variables. That does not mean the same thing as in the context of linear algebra (see linear dependence). When the covariance is normalized, one obtains the correlation matrix. From it, one can obtain the Pearson coefficient, which gives us the goodness of the fit for the best possible linear function describing the relation between the variables. In this sense covariance is a linear gauge of dependence.

See also

• Correlation
• Covariance and correlation
• Covariance function
• Covariance matrix
• Law of total covariance
• Autocovariance
• Analysis of covariance
• Sample mean and sample covariance
• Variance

External links

• MathWorld page on calculating the sample covariance