zondag 11 januari 2009

Observables

Observables are (represented by) hermitian operators.
Two observables are incompatible if and only if their commutator is nonzero i.e. incompatible observables do not commute.

A hermitian operator is a linear operator.
The corresponding (orthogonal) eigenvectors and (real) eigenvalues represent possible system states and corresponding possible outcomes for that observable.

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