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Why measurements are made of effects

Tobias Fritz

TL;DR

This work addresses why measurements in physical theories are modeled as tuples of effects summing to a unit by introducing generalized measurement theories (GMTs) where measurements are primitive and states are derived. It demonstrates that in GMTs which are probabilistically separated, each measurement is representable as a normalized tuple of effects within an associated GPT of probabilistic states, providing a principled explanation for the prevalent effect-valued description in quantum theory. It further characterizes classical GMTs as precisely those arising from Boolean algebras, showing that strongly classical and projective GMTs correspond to $\mathcal{M}_{\mathcal{B}}$ and that projectivity discriminates between Boolean-algebra based classical measurements and quantum POVMs. Overall, the framework unifies classical, quantum, and more general measurement formalisms and clarifies when the effect-tuple description must hold, with implications for foundational questions in quantum theory and GPT reconstructions.

Abstract

Both in quantum theory and in general probabilistic theories, measurements with $n$ outcomes are modelled as $n$-tuples of \emph{effects} summing up to the unit effect. Why is this the case, and can this assumption be meaningfully relaxed? Here we develop \emph{generalized measurement theories (GMTs)} as a mathematical framework for physical theories that is complementary to general probabilistic theories, and where this kind of question can be made precise and answered. We then give a definition of \emph{probabilistic state} on a GMT, prove that measurements are made of effects in every GMT in which the probabilistic states separate the measurements, and also argue that this separation condition is physically well-motivated. Finally, we also discuss when a GMT should be considered classical and characterize GMTs corresponding to Boolean algebras as those that are strongly classical and projective.

Why measurements are made of effects

TL;DR

This work addresses why measurements in physical theories are modeled as tuples of effects summing to a unit by introducing generalized measurement theories (GMTs) where measurements are primitive and states are derived. It demonstrates that in GMTs which are probabilistically separated, each measurement is representable as a normalized tuple of effects within an associated GPT of probabilistic states, providing a principled explanation for the prevalent effect-valued description in quantum theory. It further characterizes classical GMTs as precisely those arising from Boolean algebras, showing that strongly classical and projective GMTs correspond to and that projectivity discriminates between Boolean-algebra based classical measurements and quantum POVMs. Overall, the framework unifies classical, quantum, and more general measurement formalisms and clarifies when the effect-tuple description must hold, with implications for foundational questions in quantum theory and GPT reconstructions.

Abstract

Both in quantum theory and in general probabilistic theories, measurements with outcomes are modelled as -tuples of \emph{effects} summing up to the unit effect. Why is this the case, and can this assumption be meaningfully relaxed? Here we develop \emph{generalized measurement theories (GMTs)} as a mathematical framework for physical theories that is complementary to general probabilistic theories, and where this kind of question can be made precise and answered. We then give a definition of \emph{probabilistic state} on a GMT, prove that measurements are made of effects in every GMT in which the probabilistic states separate the measurements, and also argue that this separation condition is physically well-motivated. Finally, we also discuss when a GMT should be considered classical and characterize GMTs corresponding to Boolean algebras as those that are strongly classical and projective.
Paper Structure (5 sections, 11 theorems, 57 equations)

This paper contains 5 sections, 11 theorems, 57 equations.

Key Result

Lemma 2.8

Every GMT $\mathcal{M}$ comes equipped with canonical maps which are natural in $X$ in the sense that for all $f : X \to Y$, the diagram \begin{tikzcd} X \arrow[r, "\delta_X"] \arrow[d, "f"'] & \measfun(X) \arrow[d, "\measfun(f)"] \\ Y \arrow[r, "\delta_Y"'] & \measfun(Y) \end{tikzcd}commutes.

Theorems & Definitions (44)

  • Example 1.1
  • Remark 1.3
  • Definition 2.1
  • Remark 2.2
  • Example 2.3: Effect algebras
  • Example 2.4: Projective measurements
  • Example 2.5: Classical measurements
  • Example 2.6: Probabilistic measurements and random functions
  • Example 2.7: Sub-GMTs
  • Lemma 2.8
  • ...and 34 more