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Equation 90 · The Atlas That Refuses to Close

What does this equation mean?

Aw=⟨f∣A^∣ψ⟩⟨f∣ψ⟩,A_w = \frac{\langle f|\hat A|\psi\rangle}{\langle f|\psi\rangle},

Read the formula alongside the article passage below. Each part has a deeper page with its role in the equation, the supporting passage and nearby citations.

Start withlangle f|hat A|psirangle
Divide bylangle f|psirangle
This relates toA_w
How to read the two sides of this formula. Follow the article passage for the meaning of each quantity.

This equation states an equality: the expressions on both sides have the same value under the article’s assumptions. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.

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AwA_w

Symbol A_w

conditioned on that postselection.

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ff

Symbol f

f is an input to the expression that computes the quantity on the left.

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A^\hat A

Symbol hat A

the weak value of any observable.

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ψ\psi

Symbol psi

psi is an input to the expression that computes the quantity on the left.

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=

=

The expressions on both sides represent the same quantity under the stated assumptions.

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fraction

fraction

Divide the expression above the line by the one below it.

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subscript

subscript

The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.

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⟨f∣A^∣ψ⟩\langle f|\hat A|\psi\rangle

Numerator: langle f|hat A|psirangle

The complete quantity above the fraction bar.

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⟨f∣ψ⟩\langle f|\psi\rangle

Denominator: langle f|psirangle

The complete quantity below the fraction bar; it must be nonzero for this division.

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How to interpret it

With a fixed numerator, increasing a nonzero denominator reduces the fraction. Read it with the definitions, units, and assumptions supplied by the article.

What the article says around this equation

There is a fifth kind of answer to “where,” and it is worth stating precisely how it differs from all four above before using it. Prepare a system in a state |ψ\psi⟩\rangle , couple it weakly to a pointer, and then postselect on a final state |f⟩\rangle measured after the coupling. The weak value of any observable A^\hat A , position among them, conditioned on that postselection is Aw=⟨f∣A^∣ψ⟩⟨f∣ψ⟩A_w = \frac{\langle f|\hat A|\psi\rangle}{\langle f|\psi\rangle}. introduced by Aharonov, Albert, and Vaidman as the quantity a weakly coupled pointer’s mean shift actually reports, to leading order in the coupling strength, once the postselection has been performed [ 11 ] . AwA_w is not an eigenvalue of A^\hat A , not an expectation value in the ordinary sense, and…
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There is a fifth kind of answer to “where,” and it is worth stating precisely how it differs from all four above before using it. Prepare a system in a state |ψ\psi⟩\rangle , couple it weakly to a pointer, and then postselect on a final state |f⟩\rangle measured after the coupling. The weak value of any observable A^\hat A , position among them, conditioned on that postselection is Aw=⟨f∣A^∣ψ⟩⟨f∣ψ⟩A_w = \frac{\langle f|\hat A|\psi\rangle}{\langle f|\psi\rangle}. introduced by Aharonov, Albert, and Vaidman as the quantity a weakly coupled pointer’s mean shift actually reports, to leading order in the coupling strength, once the postselection has been performed [ 11 ] . AwA_w is not an eigenvalue of A^\hat A , not an expectation value in the ordinary sense, and not guaranteed to be real: it is built from an amplitude ratio over a sub-ensemble selected by an event, the postselection, that has not yet happened at the time the weak coupling acts.

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Sources cited in the surrounding passage

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