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In [[probability theory]], for a [[probability measure]] '''P''' on a [[Hilbert space]] ''H'' with [[inner product]] <math>\langle \cdot,\cdot\rangle </math>, the '''covariance''' of '''P''' is the [[bilinear form]] Cov:&nbsp;''H''&nbsp;&times;&nbsp;''H''&nbsp;→&nbsp;'''R''' given by


:<math>\mathrm{Cov}(x, y) = \int_{H} \langle x, z \rangle \langle y, z \rangle \, \mathrm{d} \mathbf{P} (z)</math>


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


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:<math>\mathrm{Cov}(x, y) = \langle Cx, y \rangle</math>
 
(from the [[Riesz representation theorem]], such operator exists if Cov is [[Bilinear form#On normed vector spaces|bounded]]). Since Cov is symmetric in its arguments, the covariance operator is
[[self-adjoint operator|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 (mathematics)|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''<sup>#</sup>, defined by
 
:<math>\mathrm{Cov}(x, y) = \int_{B} \langle x, z \rangle \langle y, z \rangle \, \mathrm{d} \mathbf{P} (z)</math>
 
where <math> \langle x, z \rangle </math> 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
 
:<math>\mathrm{Cov}(x, y) = \int z(x) z(y) \, \mathrm{d} \mathbf{P} (z) = E(z(x) z(y))</math>
 
where ''z''(''x'') is now the value of the function ''z'' at the point ''x'', i.e., the value of the [[linear functional]] <math> u \mapsto u(x) </math> evaluated at ''z''.
 
 
{{probability-stub}}
 
[[Category:Probability theory]]
[[Category:Covariance and correlation]]
[[Category:Bilinear forms]]

Revision as of 23:04, 16 January 2014

In probability theory, for a probability measure P on a Hilbert space H with inner product ,, the covariance of P is the bilinear form Cov: H × H → R given by

Cov(x,y)=Hx,zy,zdP(z)

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

Cov(x,y)=Cx,y

(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

Cov(x,y)=Bx,zy,zdP(z)

where x,z 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

Cov(x,y)=z(x)z(y)dP(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 uu(x) evaluated at z.


Template:Probability-stub