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Equation 1 · Comparing the Main Approaches to Quantum Foundations and Measurement

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P(a)=∣⟨a∣ψ⟩∣2P(a) = |\langle a \mid \psi \rangle|^2

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Inputs and operations|langle a mid psi rangle|^2
Result or conditionP(a)
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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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PP

Symbol P

P is part of the quantity the equation computes from the expression on the right.

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aa

Symbol a

a is an argument of the function-like quantity on the left; its role is set by that function’s stated inputs.

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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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superscript

superscript

A raised number can be a power. When it is a label or bound, it selects a case or the upper limit of a sum; the formula’s structure distinguishes these uses.

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Start with the settled part, because it is smaller than most accounts suggest and it is worth stating precisely. Quantum mechanics gives the Born rule: the probability of a measurement outcome is the squared modulus of a probability amplitude, P(a)=∣⟨a∣ψ⟩∣2P(a) = |\langle a \mid \psi \rangle|^2. for a system in state |ψ\psi⟩\rangle measured in a basis containing |a⟩\rangle . Every interpretation discussed here reproduces this rule for every experiment that has actually been performed. That includes Bell tests. John Bell showed in 1964 that any theory obeying two assumptions — that a measurement’s outcome depends only on a hidden variable carried by the particle and on the local setting of its own detector, not on the distant…
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Start with the settled part, because it is smaller than most accounts suggest and it is worth stating precisely. Quantum mechanics gives the Born rule: the probability of a measurement outcome is the squared modulus of a probability amplitude, P(a)=∣⟨a∣ψ⟩∣2P(a) = |\langle a \mid \psi \rangle|^2. for a system in state |ψ\psi⟩\rangle measured in a basis containing |a⟩\rangle . Every interpretation discussed here reproduces this rule for every experiment that has actually been performed. That includes Bell tests. John Bell showed in 1964 that any theory obeying two assumptions — that a measurement’s outcome depends only on a hidden variable carried by the particle and on the local setting of its own detector, not on the distant detector’s setting — predicts correlations between two separated measurements that are bounded above by a fixed value [ 1 ] . Quantum mechanics predicts correlations that exceed that bound for entangled pairs. This is a fact, not an interpretation: it was measured, most decisively in 2015 experiments that closed the two major escape routes at once — the “locality loophole,” by switching each detector’s setting after the entangled pair had already left the source, so no sub-light-speed signal could coordinate the two sides, and the “detection loophole,” by catching a high enough fraction of the pairs that a hidden mechanism selectively revealing only pairs that would violate the bound could be ruled out [ 2 ] . The 2022 Nobel Prize in Physics went to Alain Aspect, John Clauser, and Anton Zeilinger explicitly for this line of experiment, “for experiments with entangled photons, establishing the violation of Bell inequalities and pioneering quantum information science” [ 3 ] .

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