Cross-correlation matrix: Difference between revisions

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m added "no" (interpolation at values at point for which there are NO observations)
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:<math>C_{ij}(s,t) = \operatorname{corr}( X_i(s), X_j(t) )</math>
 
or a scalar, which is the trace of this matrix. If the [[probability distribution]] has any target space symmetries, i.e. symmetries in the value space of the stochastic variable (also called '''internal symmetries'''), then the correlation matrix will have induced symmetries. IfSimilarly, if there are symmetries of the space (or time) ___domain in which the random variables exist (also called '''[[spacetime symmetries]]'''), then the correlation matrixfunction will have specialcorresponding propertiesspace or time symmetries. Examples of important spacetime symmetries are &mdash;
*'''translational symmetry''' yields ''C''(''s'',''s''<nowiki>'</nowiki>) = ''C''(''s''&nbsp;&minus;&nbsp;''s''<nowiki>'</nowiki>) where ''s'' and ''s''<nowiki>'</nowiki> are to be interpreted as vectors giving coordinates of the points
*'''rotational symmetry''' in addition to the above gives ''C''(''s'', ''s''<nowiki>'</nowiki>) = ''C''(|''s''&nbsp;&minus;&nbsp;''s''<nowiki>'</nowiki>|) where |''x''| denotes the norm of the vector ''x'' (for actual rotations this is the Euclidean or 2-norm).