Every real symmetric matrix satisfying for every real vector is the covariance matrix of a random vector taking only finitely many values. The stated inequality means that is a positive semidefinite matrix. One does not need a multivariate normal distribution to realize a specified second-moment geometry. Conversely, a proposed covariance matrix must be positive semidefinite, since is the variance of the projection onto any real vector .
Here is an explicit construction. If is the matrix rank of , orthogonal diagonalization gives a real matrix with
Let be independent Rademacher random variables, each equal to or with probability , and put . Then and , so
The random vector has at most possible values. Adding any constant vector prescribes its mean without changing its covariance matrix. If , the constant vector alone suffices.
For an original two-dimensional example choose
The four equally likely values of are
Their coordinate means vanish. Their squared first coordinates average to , their squared second coordinates to , and their coordinate products to . The displayed covariance matrix is therefore realized exactly, without sampling error or an asymptotic argument.
These four values are a complete probability model with masses , not automatically an independent random sample whose population is unknown. Applying the usual divisor-three sample covariance matrix to the same four rows would give . NIST explicitly distinguishes that unbiased sample formula with divisor ; probability-weighted population moments use the assigned masses instead.[ref]
The sign construction need not minimize the number of points. If a distribution has positive-mass support points, the centered points obey one nontrivial weighted relation, so their span has dimension at most . Its covariance matrix consequently has matrix rank at most , requiring when . Matching a covariance matrix also does not match the full probability distribution: this finite model and a continuous Gaussian model can have identical means and covariances while assigning very different probabilities to nonlinear events.

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