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Physical Review

Undecidability of Macroscopically Distinguishable States in Quantum Field Theory

Arthur B. Komar

Published Jan 27, 1964• 56 citations
Publisher

Abstract

A heuristic discussion is presented regarding quantum field theory as a synthesis of the complementary theories of classical mechanics and quantum mechanics. If the states of quantum field theory are partitioned in equivalence classes accordingly as their occupation numbers differ in a finite or an infinite number of places, it is suggested that we define states to be macroscopically distinguishable if they belong to different equivalence classes. It is then proven that there is, in general, no effective procedure for determining whether or not two arbitrarily given states of a quantum system having an infinite number of degrees of freedom are macroscopically distinguishable.

DOI
10.1103/physrev.133.b542

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A heuristic discussion is presented regarding quantum field theory as a synthesis of the complementary theories of classical mechanics and quantum mechanics. If the states of quantum field theory are partitioned in equivalence classes accordingly as their occupation numbers differ in a finite or an infinite number of places, it is suggested that we define states to be macroscopically distinguishable if they belong to different equivalence classes. It is then proven that there is, in general, no effective procedure for determining whether or not two arbitrarily given states of a quantum system having an infinite number of degrees of freedom are macroscopically distinguishable.
Philosophical debate on the measurement problem of quantum mechanics has, for the most part, been confined to the non-relativistic version of the theory. Quantizing quantum field theory, or making quantum mechanics relativistic, yields a conceptual framework capable of dealing with the creation and annihilation of an indefinite number of particles in interaction with fields, i.e. quantum systems with an infinite number of degrees of freedom. I want to show that a solution to the standard measurement problem is available if we exploit the properties of the infinite quantum models available in this broader conceptual framework. There is a qualitative difference between quantum systems with an infinite number of degrees of freedom and quantum systems with a finite number of degrees of freedom. In the infinite case, there exist many unitarily inequivalent irreducible Hilbert space representations of the algebra of observables of the system. In the finite case, there is only one such representation.
Abstract The condition for distinguishability of a countably infinite number of pure states by a single measurement is given. Distinguishability is to be understood as the possibility of an unambiguous measurement. For a finite number of states, it is known that the necessary and sufficient condition of distinguishability is that the states are linearly independent. For an infinite number of states, several natural classes of distinguishability can be defined. We give a necessary and sufficient condition for a system of pure states to be distinguishable. It turns out that each level of distinguishability naturally corresponds to one of the generalizations of linear independence to families of infinite vectors. As an important example, we apply the general theory to von Neumann’s lattice, a subsystem of coherent states which corresponds to a lattice in the classical phase space. We prove that the condition for distinguishability is that the area of the fundamental region of the lattice is greater than the Planck constant, and also find subtle behavior on the threshold. These facts reveal the measurement theoretical meaning of the Planck constant and give a justification for the interpretation that it is the smallest unit of area in the phase space. The cases of uncountably many states and of mixed states are also discussed.
The therapeutic approach to quantum theory developed here is meant to be applicable not only to non-relativistic quantum mechanics, but to more advanced quantum theories as well. More specifically, it is meant to be applicable to the quantum theories of systems with infinitely many degrees of freedom, quantum field theories in particular. However, the quantum theories of systems with infinitely many degrees of freedom harbour additional philosophical challenges besides those that are already present in non-relativistic quantum mechanics, and it is to be hoped that the approach suggested here may help to clarify and address those challenges as well. The present chapter turns to some aspects of the interpretation of quantum field theory and assesses them in the light of the Rule Perspective. These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.
We discuss the q deformation of Weyl-Heisenberg algebra in connection with the von Neumann theorem in Quantum Mechanics. We show that the q-deformation parameter labels the Weyl systems in Quantum Mechanics and the unitarily inequivalent representations of the canonical commutation relations in Quantum Field Theory. The von Neumann theorem in Quantum Mechanics (QM) states that for systems with finite number of degrees of freedom the representations of the canonical commutation relations (ccr), also called the Weyl representations, are each other unitarily equivalent. In the limit of infinite number of degrees of freedom, namely in Quantum Field Theory
Abstract According to a regnant criterion of physical equivalence for quantum theories, a quantum field theory (QFT) typically admits continuously many physically inequivalent realizations. This, the second of a two‐part introduction to topics in the philosophy of QFT, continues the investigation of this alarming circumstance. It begins with a brief catalog of quantum field theoretic examples of this non‐uniqueness, then presents the basics of the algebraic approach to quantum theories, which discloses a structure common even to ‘physically inequivalent’ realizations of a QFT. Finally, it introduces and evaluates a handful of strategies for interpreting quantum theories in the face of the non‐uniqueness of their Hilbert space representations.
This work analyzes the fundamental distinction between finite-dimensional quantum systems and infinite-dimensional wavefunction systems. It introduces three mathematically independent notions of dimension—linear dimension, parameter dimension, and degree-of-freedom dimension—and shows that finite-dimensional systems are “triple-finite,” while wavefunction systems such as L^2(R) are “triple-infinite.” The paper distinguishes geometric continuity on finite-dimensional projective manifolds (e.g., the Bloch sphere) from structural continuity arising from the uncountable degrees of freedom of continuous configuration spaces. It further explains why infinite-dimensional systems cannot be reduced to finite-dimensional ones, drawing on functional analysis, spectral theory, and the properties of unbounded operators. Intermediate systems such as L^2([0,L]) and the extension to quantum field theory are also discussed, illustrating how spatial topology shapes spectral and dynamical behavior. The framework clarifies the categorical difference between finite- and infinite-dimensional quantum state spaces and highlights their complementary roles in quantum theory. 本文系统分析了有限维量子系统与无限维波函数系统之间的根本差异。文章提出三种彼此独立的“维度”概念——线性维度、参数维度与自由度维度,并指出有限维系统是“三重有限”,而波函数系统(如 L^2(R))是“三重无限”。有限维系统的连续性来自射影流形的几何结构(如 Bloch 球),而无限维系统的连续性来自连续构型空间所带来的不可数自由度。文章进一步利用泛函分析与谱理论论证了无限维系统对有限维系统的不可约化性,并讨论了中间系统 L^2([0,L]) 以及量子场论中的更高层次结构连续性。该框架揭示了有限维与无限维量子态空间在范畴上的本质差异,并说明它们在量子理论中所扮演的互补角色。