nLab wave function collapse

Contents

Context

Quantum systems

quantum logic


quantum physics


quantum probability theoryobservables and states


quantum information


quantum computation

quantum algorithms:

Contents

Idea

In the context of quantum mechanics, the collapse of the wave function, also known as the reduction of the wave packet, is said to occur after observation or measurement, when a wave function expressed as the sum of eigenfunctions of the observable is projected randomly onto one of them. Different interpretations of quantum mechanics understand this process differently.

The perspective associated with the Bayesian interpretation of quantum mechanics observes (see below) that the apparent collapse is just the mathematical reflection of the formula for conditional expectation values in quantum probability theory.

Relation to conditional expectation values

There is a close relation between wave function collapse and conditional expectation values in quantum probability (e.g. Kuperberg 05, section 1.2, Yuan 12):

Let (𝒜,)(\mathcal{A},\langle -\rangle) be a quantum probability space, hence a complex star algebra 𝒜\mathcal{A} of quantum observables, and a state on a star-algebra :𝒜\langle -\rangle \;\colon\; \mathcal{A} \to \mathbb{C}.

This means that for A𝒜A \in \mathcal{A} any observable, its expectation value in the given state is

𝔼(A)A. \mathbb{E}(A) \;\coloneqq\; \langle A \rangle \in \mathbb{C} \,.

More generally, if P𝒜P \in \mathcal{A} is a real idempotent/projector

(1)P *=P,AAAPP=P P^\ast = P \,, \phantom{AAA} P P = P

thought of as an event, then for any observable A𝒜A \in \mathcal{A} the conditional expectation value of AA, conditioned on the observation of PP, is (e.g. Redei-Summers 06, section 7.3, see also Fröhlich-Schubnel 15, (5.49), Fröhlich 19 (45))

(2)𝔼(A|P)PAPP. \mathbb{E}(A \vert P) \;\coloneqq\; \frac{ \left \langle P A P \right\rangle }{ \left\langle P \right\rangle } \,.

Now assume a star-representation ρ:𝒜End()\rho \;\colon\; \mathcal{A} \to End(\mathcal{H}) of the algebra of observables by linear operators on a Hilbert space \mathcal{H} is given, and that the state \langle -\rangle is a pure state, hence given by a vector ψ\psi \in \mathcal{H} (“wave function”) via the Hilbert space inner product (),():\langle (-), (-)\rangle \;\colon\; \mathcal{H} \otimes \mathcal{H} \to \mathbb{C} as

A ψ|A|ψ ψ,Aψ. \begin{aligned} \langle A \rangle & \coloneqq \left\langle\psi \vert A \vert \psi \right\rangle \\ & \coloneqq \left\langle\psi, A \psi \right\rangle \end{aligned} \,.

In this case the expression for the conditional expectation value (2) of an observable AA conditioned on an idempotent observable PP becomes (notationally suppressing the representation ρ\rho)

𝔼(A|P) =ψ|PAP|ψψ|P|ψ =Pψ|A|PψPψ|Pψ, \begin{aligned} \mathbb{E}(A\vert P) & = \frac{ \left\langle \psi \vert P A P\vert \psi \right\rangle }{ \left\langle \psi \vert P \vert \psi \right\rangle } \\ & = \frac{ \left\langle P \psi \vert A \vert P \psi \right\rangle }{ \left\langle P \psi \vert P \psi \right\rangle } \,, \end{aligned}

where in the last step we used (2).

This says that assuming that PP has been observed in the pure state |ψ\vert \psi\rangle, then the corresponding conditional expectation values are the same as actual expectation values but for the new pure state |Pψ\vert P \psi \rangle.

This is the statement of “wave function collapse”

|ψP|ψ. \vert \psi \rangle \mapsto P \vert \psi \rangle \,.

The original wave function is ψ\psi \in \mathcal{H}, and after observing PP it “collapses” to PψP \psi \in \mathcal{H} (up to normalization).

quantum probability theoryobservables and states

References

Early explicit discussion of wavefunction collapse in quantum measurements, including discussion relating to historical experiments:

But the formulation in von Neumann 1932 postulated that a pure state would collapse to a mixed state when the quantum observable‘s eigenvalues are degenerate.

This problem was pointed out and the modern formulation of the collapse postulate was formulated by:

Textbook accounts in quantum information theory:

Discussion from the point of view of quantum probability includes

See also

Last revised on October 27, 2022 at 12:22:05. See the history of this page for a list of all contributions to it.