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Nuclear Physics B - Proceedings Supplements

Classical measurements on a quantum mechanical system

Willis E. Lamb

Published Mar 1, 1989• 9 citations
Publisher
DOI
10.1016/0920-5632(89)90438-6

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Completing the Quantum Measurement Problem Through the Carlo Framework: A Mechanism for Collapse, Definiteness, and Classical Emergence

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This work completes the quantum measurement problem by supplying the mechanism standard quantum mechanics lacks. The theory contains two incompatible evolution rules: continuous unitary evolution and discontinuous measurement collapse. Quantum mechanics does not explain how collapse is triggered, why a single outcome is selected, or how classical definiteness emerges. Using the Carlo Framework, this paper introduces the contradiction engine, the trajectory update rule, and the Reset Operator > as the missing structural components that mechanise collapse. The completed model treats measurement as a contradiction loop between superposed and classical states. When this loop exceeds tolerance, the Carlo reset mechanism produces a definite classical outcome. This paper formalises the measurement contradiction, defines the collapse threshold, and provides a unified mechanism linking quantum evolution to classical results. KEYWORDS:quantum measurement problem, wavefunction collapse, unitary evolution, quantum mechanics, contradiction engine, Carlo Framework, Reset Operator, trajectory update rule, superposition, classical emergence, decoherence, measurement theory, quantum foundations, quantum-classical boundary, collapse dynamics, threshold mechanisms, contradiction loops, system evolution, dynamic collapse, structural completion, mechanism-level explanation, quantum state reduction, contextual measurement, quantum information, quantum interpretation, foundational physics, theoretical physics, dynamic systems, system reorganisation, emergent classicality, contradiction-driven change, collapse operator, measurement dynamics, quantum modelling, conceptual engineering, physics foundations, quantum behaviour, system reset events, structural dynamics, quantum transitions, measurement interaction, outcome selection, classical definiteness, quantum paradoxes, dynamic resolution, system transformation

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Measurements in quantum mechanics

Henry Margenau

Annals of Physics•Jun 1, 1963•5 citations

The Quantum-like Face of Classical Mechanics

Partha Ghose

It is first shown that when the Schrödinger equation for a wave function is written in the polar form, complete information about the system's {\em quantum-ness} is separated out in a single term $Q$, the so called `quantum potential'. An operator method for classical mechanics described by a `classical Schrödinger equation' is then presented, and its similarities and differences with quantum mechanics are pointed out. It is shown how this operator method goes beyond standard classical mechanics in predicting coherent superpositions of classical states but no interference patterns, challenging deeply held notions of classical-ness, quantum-ness and macro realism. It is also shown that measurement of a quantum system with a classical measuring apparatus described by the operator method does not have the measurement problem that is unavoidable when the measuring apparatus is quantum mechanical. The type of decoherence that occurs in such a measurement is contrasted with the conventional decoherence mechanism. The method also provides a more convenient basis to delve deeper into the area of quantum-classical correspondence and information processing than exists at present.

arXiv:1801.02499•Jan 5, 2018•1 citation

Classicality in Quantum Mechanics

Olaf Dreyer

In this article we propose a solution to the measurement problem in quantum mechanics. We point out that the measurement problem can be traced to an a priori notion of classicality in the formulation of quantum mechanics. If this notion of classicality is dropped and instead classicality is defined in purely quantum mechanical terms the measurement problem can be avoided. We give such a definition of classicality. It identifies classicality as a property of large quantum system. We show how the probabilistic nature of quantum mechanics is a result of this notion of classicality. We also comment on what the implications of this view are for the search of a quantum theory of gravity.

•Nov 7, 2006•3 citations

Measurements in quantum mechanics

Henry Margenau

Annals of Physics•Sep 1, 1963•113 citations
This work completes the quantum measurement problem by supplying the mechanism standard quantum mechanics lacks. The theory contains two incompatible evolution rules: continuous unitary evolution and discontinuous measurement collapse. Quantum mechanics does not explain how collapse is triggered, why a single outcome is selected, or how classical definiteness emerges. Using the Carlo Framework, this paper introduces the contradiction engine, the trajectory update rule, and the Reset Operator > as the missing structural components that mechanise collapse. The completed model treats measurement as a contradiction loop between superposed and classical states. When this loop exceeds tolerance, the Carlo reset mechanism produces a definite classical outcome. This paper formalises the measurement contradiction, defines the collapse threshold, and provides a unified mechanism linking quantum evolution to classical results. KEYWORDS:quantum measurement problem, wavefunction collapse, unitary evolution, quantum mechanics, contradiction engine, Carlo Framework, Reset Operator, trajectory update rule, superposition, classical emergence, decoherence, measurement theory, quantum foundations, quantum-classical boundary, collapse dynamics, threshold mechanisms, contradiction loops, system evolution, dynamic collapse, structural completion, mechanism-level explanation, quantum state reduction, contextual measurement, quantum information, quantum interpretation, foundational physics, theoretical physics, dynamic systems, system reorganisation, emergent classicality, contradiction-driven change, collapse operator, measurement dynamics, quantum modelling, conceptual engineering, physics foundations, quantum behaviour, system reset events, structural dynamics, quantum transitions, measurement interaction, outcome selection, classical definiteness, quantum paradoxes, dynamic resolution, system transformation
It is first shown that when the Schrödinger equation for a wave function is written in the polar form, complete information about the system's {\em quantum-ness} is separated out in a single term QQQ, the so called `quantum potential'. An operator method for classical mechanics described by a `classical Schrödinger equation' is then presented, and its similarities and differences with quantum mechanics are pointed out. It is shown how this operator method goes beyond standard classical mechanics in predicting coherent superpositions of classical states but no interference patterns, challenging deeply held notions of classical-ness, quantum-ness and macro realism. It is also shown that measurement of a quantum system with a classical measuring apparatus described by the operator method does not have the measurement problem that is unavoidable when the measuring apparatus is quantum mechanical. The type of decoherence that occurs in such a measurement is contrasted with the conventional decoherence mechanism. The method also provides a more convenient basis to delve deeper into the area of quantum-classical correspondence and information processing than exists at present.
In this article we propose a solution to the measurement problem in quantum mechanics. We point out that the measurement problem can be traced to an a priori notion of classicality in the formulation of quantum mechanics. If this notion of classicality is dropped and instead classicality is defined in purely quantum mechanical terms the measurement problem can be avoided. We give such a definition of classicality. It identifies classicality as a property of large quantum system. We show how the probabilistic nature of quantum mechanics is a result of this notion of classicality. We also comment on what the implications of this view are for the search of a quantum theory of gravity.