Assuming that the evolution of the Quantum State of the Universe may be simulated by the Schrödinger equation, Kolmogorov’s theory of Algorithmic Probability provides us with an elegant mathematical description of what a particular physicist observes during a Quantum Measurement.
Assuming that the evolution of the Quantum State of the Universe may be simulated by the Schrödinger equation, Kolmogorov’s theory of Algorithmic Probability provides us with an elegant mathematical description of what a particular physicist observes during a Quantum Measurement. Interestingly, this description of non-computable measurements is in qualitative agreement with the Von Neumann-Wigner theory of Quantum Measurement.
If an observer is a purely physical object, a more comprehensive wave function may now be expressed which encompasses both the state of the Quantum system being observed and the state of the observer. The various possible measurements are now in a superposition of states, representing different observations. However, this leads to a problem: you would now need another measuring device to collapse this larger wave function but this would develop into a superposition state. Another device would be needed to collapse this state ad infinitum. This problem-the Von Neumann chain-is an infinite regression of measuring devices whose stopping point is presumed to be the conscious mind.-Aeowyn Kendall
Von Neumann’s theory of Quantum measurement may thus be summarised as follows:
The Quantum state of a system generally evolves smoothly as dictated by the Schrödinger wave equation.
Otherwise, the Quantum State of this system collapses suddenly and sharply due to a conscious observer.
If we consider that there is a Quantum State associated with the Universe and combine this with the Kantian view that the mind interprets the world, then what a person observes may be defined by the Algorithmic Probability:
\[\begin{equation} P(x|\hat{x})= 2^{-K_U(x\hat{x})} \tag{1} \end{equation}\]
where \(\hat{x}\) denotes the Qualia or conscious state of a person and \(x\) denotes the observations of this person. As Kolmogorov Complexity is not computable, what a particular physicist observes during a Quantum experiment may not be determined by a computable function such as the Schrödinger Wave equation. However, \(P\) may be approximated by a computable probability distribution \(\sum_x f(x|\hat{x}) =1\) since:
\[\begin{equation} \mathbb{E}[K_U(x|\hat{x})] = H(x|\hat{x}) + \mathcal{O}(1) \tag{2} \end{equation}\]
This allows a Quantum Physicist to predict the average outcomes of a Quantum measurement from a frequentist perspective although they can’t predict a particular outcome with certainty.
This has a number of important consequences:
Rocke (2022, Jan. 5). Kepler Lounge: Revisiting the unreasonable effectiveness of mathematics. Retrieved from keplerlounge.com
R. J. Solomonoff A formal theory of inductive inference: Parts 1 and 2. Information and Control, 7:1–22 and 224–254, 1964.
A. N. Kolmogorov Three approaches to the quantitative definition of information. Problems of Information and Transmission, 1(1):1–7, 1965
G. J. Chaitin On the length of programs for computing finite binary sequences: Statistical considerations. Journal of the ACM, 16(1):145–159, 1969.
L.A. Levin. Laws of information conservation (non-growth) and aspects of the foundation of probability theory. Problems Information Transmission, 10(3):206-210, 1974.
John A. Wheeler, 1990, “Information, physics, quantum: The search for links” in W. Zurek (ed.) Complexity, Entropy, and the Physics of Information. Redwood City, CA: Addison-Wesley.
E.T. Jaynes. Information Theory and Statistical Mechanics. The Physical Review. 1957.
von Neumann, John (1932). Mathematische Grundlagen der Quantenmechanik (Mathematical Foundations of Quantum Mechanics) Princeton University Press., . ISBN 978-0-691-02893-4.
Shannon, Claude E. (1948). A Mathematical Theory of Communication Bell System Technical Journal 27: 379-423. doi:10.1002/j.1538-7305.1948.tb01338.x.
Markus Mueller. Law without law: from observer states to physics via algorithmic information theory. Arxiv. 2020.
Gerard’t Hooft. The Cellular Automaton Interpretation of Quantum Mechanics. Arxiv. 2015.
Wigner, Eugene; Henry Margenau (1967). “Remarks on the Mind Body Question, in Symmetries and Reflections, Scientific Essays”. American Journal of Physics. 35 (12): 1169–1170.
L. A. Levin, Universal sequential search problems. Problems of Information Transmission, 9(3):265–266, 1973.
For attribution, please cite this work as
Rocke (2022, Dec. 26). Kepler Lounge: Algorithmic Probability and Wave Function collapse. Retrieved from keplerlounge.com
BibTeX citation
@misc{rocke2022algorithmic, author = {Rocke, Aidan}, title = {Kepler Lounge: Algorithmic Probability and Wave Function collapse}, url = {keplerlounge.com}, year = {2022} }