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quasi-state

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Idea

In quantum mechanics, a qausi-state on an algebra of observables A is a function ρ:A that is required to satisfy the axioms of a genuine state (linearity and positivity) only on the poset of commutative subalgebras of A.

While therefore the condition on quasi-states is much weaker than that for states, Gleason's theorem asserts that if A=B(H) for dimH>2, then all quasi-states are in fact states.

Notice that a quasi-state is naturally regarded as an actual state, but internal to the ringed topos over the poset of commutative subalgebras of A. Therefore Gleason’s theorem is one of the motivations for regarding this ringed topos as the quantum phase space (“Bohrification”.) The other is the Kochen-Specker theorem.

Revised on September 16, 2011 01:46:04 by Urs Schreiber (89.204.153.85)