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The Unmeasured Ground: Why Quantum Mechanics Cannot Explain What It Measures

Matt Prager

Published Apr 27, 2026• 0 citations
Publisher

Abstract

Quantum physics has a measurement problem, and it’s not the one the field usually means: it’s that physics has built a precise theory of measurement outcomes without a theory of what measurement structurally is. The Galley-Kent exchange makes this gap unusually visible. Galley, Masanes, and Müller argued that quantum measurement postulates follow necessarily from structural postulates plus the possibility of state estimation. Kent refuted this, constructing alternative measurement postulates consistent with those assumptions. We argue that both positions operate one level above the question that would resolve their debate: what is the minimum structure that makes any measurement coherent in the first place? We show that this floor — two faces, one non-directed comparator, and the invariant sameness that makes their difference determinate — forces complex Hilbert space as the unique minimal field consistent with its constraints, and forces the Born rule as the unique probability assignment that closes both faces simultaneously. Galley et al. are correct that measurement postulates are necessary, but the proof does not live inside quantum mechanics. Kent's alternatives are formally consistent but do not instantiate coherent measurement: they either abandon ratio structure or treat measurement as directed rather than comparative. The proof of necessity lives below quantum mechanics, not inside it.

DOI
10.5281/zenodo.19818300

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Quantum physics has a measurement problem, and it’s not the one the field usually means: it’s that physics has built a precise theory of measurement outcomes without a theory of what measurement structurally is. The Galley-Kent exchange makes this gap unusually visible. Galley, Masanes, and Müller argued that quantum measurement postulates follow necessarily from structural postulates plus the possibility of state estimation. Kent refuted this, constructing alternative measurement postulates consistent with those assumptions. We argue that both positions operate one level above the question that would resolve their debate: what is the minimum structure that makes any measurement coherent in the first place? We show that this floor — two faces, one non-directed comparator, and the invariant sameness that makes their difference determinate — forces complex Hilbert space as the unique minimal field consistent with its constraints, and forces the Born rule as the unique probability assignment that closes both faces simultaneously. Galley et al. are correct that measurement postulates are necessary, but the proof does not live inside quantum mechanics. Kent's alternatives are formally consistent but do not instantiate coherent measurement: they either abandon ratio structure or treat measurement as directed rather than comparative. The proof of necessity lives below quantum mechanics, not inside it.
Masanes, Galley and Müller \cite{masanes2019measurement} argue that the measurement postulates of non-relativistic quantum mechanics follow from the structural postulates together with an assumption they call the "possibility of state estimation". Their argument also relies on what they term a "theory-independent characterization of measurements for single and multipartite systems". We refute their conclusion, giving explicit examples of non-quantum measurement and state update rules that satisfy all their assumptions. We also show that their "possibility of state estimation" assumption is neither necessary nor sufficient to ensure a sensible notion of state estimation within a theory whose states are described by the quantum formalism. We further show their purportedly "theory-independent" characterization assumes several properties of quantum measurements that exclude plausible alternative types of measurement. We illustrate all these points with specific alternative measurement postulates and post-measurement state update rules. We conclude that, contrary to some folklore, quantum mechanics is by no means an island in theory-space. It can consistently be extended by rules for obtaining information about quantum states other than via POVMs. Whether such rules are realised in nature, for example in linking quantum theory and gravity, is an empirical question that cannot be resolved by theoretical analysis alone.
Adrian Kent has recently presented a critique \cite{Kent} of our paper \cite{MGM} in which he claims to refute our main result: the measurement postulates of quantum mechanics can be derived from the rest of postulates, once we assume that the set of mixed states of a finite-dimensional Hilbert space is finite-dimensional. To construct his argument, Kent considers theories resulting from supplementing quantum mechanics with hypothetical ``post-quantum'' measurement devices. We prove that each of these theories contains pure states (i.e. states of maximal knowledge) which are not rays of the Hilbert space, in contradiction with the ``pure state postulate'' of quantum mechanics. We also prove that these alternatives violate the finite-dimensionality of mixed states. Each of these two facts separately invalidates the refutation. In this note we also clarify the assumptions used in \cite{MGM} and discuss the notions of pure state, physical system, and the sensitivity of the structure of the state space under modifications of the measurements or the dynamics.
Adrian Kent has recently presented a critique [arXiv:2307.06191] of our paper [Nat. Comms. 10, 1361 (2019)] in which he claims to refute our main result: the measurement postulates of quantum mechanics can be derived from the rest of postulates, once we assume that the set of mixed states of a finite-dimensional Hilbert space is finite-dimensional. To construct his argument, Kent considers theories resulting from supplementing quantum mechanics with hypothetical "post-quantum" measurement devices. We prove that each of these theories contains pure states (i.e. states of maximal knowledge) which are not rays of the Hilbert space, in contradiction with the "pure state postulate" of quantum mechanics. We also prove that these alternatives violate the finite-dimensionality of mixed states. Each of these two facts separately invalidates the refutation. In this note we also clarify the assumptions used in [Nat. Comms. 10, 1361 (2019)] and discuss the notions of pure state, physical system, and the sensitivity of the structure of the state space under modifications of the measurements or the dynamics.
This article examines the scope and limitations of quantum mechanics in its Schrödinger and Dirac formulations. Quantum theory provides an extraordinarily precise description of how physical states evolve, interfere, and produce measurable probabilities. However, like other foundational theories, it presupposes a specific mathematical structure—complex Hilbert spaces, linear unitary dynamics, an external time parameter, and the Born rule—that it does not itself explain. The work argues that quantum mechanics answers the question of how quantum states behave, but not the deeper question of why physical reality admits a state-based, probabilistic description at all. To address this missing level of explanation, the article places quantum mechanics within the broader framework of the Thermodynamic Imperative of Order (TIO) and the Granular Entropic Program (GEP). Within this framework, quantum states are interpreted as emergent, statistically stable macroscopic representations of typical correlations in high-dimensional configuration spaces. Linearity, unitarity, and the Born rule arise as necessary consequences of measure concentration and stability, rather than as fundamental postulates. The article does not propose modifications to quantum mechanics. Instead, it clarifies the domain of validity of the theory and explains why a framework with its structure and remarkable universality must exist if stable quantum phenomena are to be observed at all.
This note presents a structural resolution of the quantum measurement problem by decomposing it into three distinct physical layers: the persistence of quantum coherence, the emergence of a single definite classical outcome, and the origin of quantum probability. It provides physical explanations for coherence loss and outcome definiteness based on coordination limits, thermodynamic irreversibility, and information stability, without introducing new dynamics or observer postulates. The analysis further clarifies that the Born rule does not arise from measurement or macroscopic processing, but is an irreducible structural constraint governing microscopic quantum interactions. By correctly delimiting the scope of measurement theory, the note resolves longstanding conceptual confusion while remaining fully consistent with standard quantum mechanics.