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arXiv:quant-ph/0303065

Objective vs Observer Measurements

Richard A. Mould

Published Mar 11, 2003• 2 citations
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Abstract

Post-inflationary boundary conditions are essential to the existence of our highly structured universe, and these can only come about through quantum mechanical state reductions - i.e., through measurements. The choice is between: An 'objective' measurement that allows reduction to occur independent of conscious observers, and an 'observer' based measurement that ties reduction to the existence of a conscious observer. It is shown in this paper that that choice cannot be determined empirically; so how we finally understand state reduction will be decided by the way that reduction is used in a wider (future) theoretical framework. Key Words: consciousness, decoherence, stochastic choice, wave collapse.

DOI
10.48550/arxiv.quant-ph/0303065

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Post-inflationary boundary conditions are essential to the existence of our highly structured universe, and these can only come about through quantum mechanical state reductions - i.e., through measurements. The choice is between: An 'objective' measurement that allows reduction to occur independent of conscious observers, and an 'observer' based measurement that ties reduction to the existence of a conscious observer. It is shown in this paper that that choice cannot be determined empirically; so how we finally understand state reduction will be decided by the way that reduction is used in a wider (future) theoretical framework. Key Words: consciousness, decoherence, stochastic choice, wave collapse.
We consider two straightforward rules that govern the stochastic choice in a single quantum mechanical event. They are shown to lead to absurd results if an objective state reduction is allowed to compete with an observer state reduction. Since the latter collapse is empirically verifiable, the existence of the former is thrown into question. Key Words: Born Interpretation, brain states, continuous observation, conscious observer, objective measurement, observer measurement, probability current, state reduction, wave collapse.
We examine the role of a conscious observer in a typical quantum mechanical measurement. Four rules are given that govern stochastic choice and state reduction in several cases of continuous and intermittent observation. It is found that consciousness always accompanies a state reduction leading to observation, but its presence is not sufficient to 'cause' a reduction. The distinction is clarified and codified by the rules that are given below. This is the first of several papers that lead to an experimental test of the rules, and of the "parallel principle" that is described elsewhere. Key words: Brain states, boundary conditions, consciousness, conscious observer, environment, decoherence, macroscopic superposition, measurement, state reduction, state collapse, von Neumann.
In a previous paper we examined the role of a conscious observer in a typical quantum mechanical measurement. Four rules were given that were found to govern the stochastic choice and state reduction in several cases of continuous and intermittent observation. It was shown that consciousness always accompanies a state reduction leading to observation, but its presence is not sufficient to 'cause' a reduction. The distinction is clarified and codified by the rules that are repeated below. In this paper, these rules are successfully applied to two different versions of the Schrodinger cat experiment. Key Words: Brain states, boundary conditions, cat paradox, consciousness, conscious observer, environment, decoherence, macroscopic superposition, measurement, state reduction, state collapse, von Neumann.
Several theories have been advanced recently which appear to offer a resolution to that portion of the measurement problem which previously dealt with a possible reduction of the state vector in a subjective fashion by the brain, mind or consciousness. It now appears, based on both biological and mathematical analysis, that collapse of the wave function always takes place in an objective fashion in the retinal rod-rhodopsin molecule, and that only measured information is ever presented to the brain, mind or consciousness for possible subjective analysis. The remaining portion of the measurement problem has to do with the use and legitimacy of such terms as boundary (Heisenberg or von Neumann cut), information, irreversible, measurement, microscopic, macroscopic, observer (apparatus or measuring system), observed (measured system) and wave function collapse. This portion of the measurement problem may be resolved in two ways. First, by adopting Dirac's theory that it is nature that makes the choice of measuremental result. Second, by the insertion of a mesoscopic bridge between the microscopic and macroscopic worlds, in the existing form of the rhodopsin molecule with its retinal and opsin components.
If conscious observers are to be included in the quantum mechanical universe, we need to find the rules that engage observers with quantum mechanical systems. The author has proposed five rules that are discovered by insisting on empirical completeness; that is, by requiring the rules to draw empirical information from Schrodinger's solutions that is more complete than is currently possible with the (Born) probability interpretation. I discard Born's interpretation, introducing probability solely through probability current. These rules tell us something about brains. They require the existence of observer brain states that are neither conscious nor unconscious. I call them 'ready' brain states because they are on stand-by, ready to become conscious the moment they are stochastically chosen. Two of the rules are selection rules involving ready brain states. The place of these rules in a wider theoretical context is discussed. Key Words: boundary conditions, consciousness, decoherence, macroscopic superposition, Penrose, state reduction, von Neumann, wave collapse.