Submitted:
09 September 2025
Posted:
10 September 2025
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Abstract
Keywords:
1. Introduction
2. Overview of Some Philosophical Approaches to the Mind-Body Problem
3. Model for Elementary Consciousness in a Fundamental Particle
4. Measurement, Observation, and Wigner’s Friend-like Scenarios
5. The Combination Problem: Generating Consciousness in a Composite System
6. Doing-Otherwise Mechanism in DAQM: Consciousness Backaction on Physical Space
7. The Road from Elementary Microscopic Proto-Consciousness to Consciousness in Complex Biological Macroscopic Systems
8. Conclusions
Appendix A. Overview of the Darwinian Approach to Quantum Mechanics (DAQM)
Appendix A.1. Regulating Principle: Increase of Survival Information Complexity
Appendix A.2. Discussion on the Derivation of the Postulates of Quantum Mechanics
Appendix A.2.1. Data Storage: Complex Wave Function
Appendix A.2.2. Data Retrieval and Processing: Hilbert Space Structure
Appendix A.2.3. Further Data Processing: Schrödinger Equation
Appendix A.2.4. Output Computing: Guiding Equation
Appendix A.3. Computing Quantum Behaviour in Real Time: Simulation of Closed Timelike Curves (CTCs) on Information Spaces
Appendix A.4. Bell Inequality Violations in DAQM
Appendix A.5. Generating Anticipation Modules on Information Spaces
Appendix A.6. Conclusions
| 1 | This module will play a central role in the characterization of consciousness in the information-theoretic model of a fundamental particle in DAQM as will be mentioned bellow. |
| 2 | The function of the enumerated elements that are stored on the information space will be further analysed in the Appendix. |
| 3 | The possible fundamental relationship between irreversibility and consciousness has been highlighted by Aaronson (2014). |
| 4 | Nevertheless, although the DAQM is then a realist approach as the de Broglie-Bohm theory, in contraposition to the patent nonlocality of the latter, DAQM is a local theory, as will be further discussed in the Appendix. |
| 5 | Notice that in this elementary Wigner’s friend-like scenario the Wigner’s friend particle f does not measure the test particle s (as it is considered in standard Wigner´s friend scenarios), but it just observes the location occupied by the test particle as a consequence of that the Wigner’s friend particle itself is being measured, and therefore, according to the DAQM model, it becomes an observer. In addition, as has been mentioned, an elementary Wigner´s friend particle f and an elementary Wigner particle w cannot communicate between them. |
| 6 | Note, however, that, in DAQM, as in Bohmian mechanics, the result of any measurement would be given in terms of positions of particles or positions of pointers in the measurement apparatus. |
| 7 | The possibility that in certain regions or domains a different equilibrium might have been reached should be contemplated as a possible test for DAQM. |
| 8 | This mechanism has already been proposed by Penrose (2023) to explain free will, but assuming a real backward in time causation. |
| 9 | More elaborated definitions of may be considered for a detailed technical analysis (e.g., including elements of anticipation depth or incorporating a minimum value for denominators to avoid singularities, etc.), but the adopted definition seemingly captures the essentials for a conceptual discussion. |
| 10 | The quantum advantage is the capacity of a quantum computer for solving in polynomial time, when specific appropriate quantum algorithms have been developed, certain exponentially computational complex problems for classical computers. |
| 11 | Closed timelike curves are possible theoretical solutions of general relativity field equations representing loop paths through spacetime that return to a prior event in the worldline. |
| 12 | The “grandfather paradox” refers to the illogical situation that the presence of a CTC raises. A time traveller voyaging through a CTC might hypothetically kill his own grandfather precluding his own existence. |
| 13 | The Bell inequality establishes a mathematical constraint on the correlations of the outcomes of measurements on two spatially separated parts of a system assuming local causality (also named Bell locality condition or factorizability) and certain supplementary assumptions. Bell inequality violations are then the consequence of nonclassical correlations predicted by the quantum mechanical formalism and experimentally observed in specific setups involving spatially separated parts of composite systems for certain states of such systems. See Myrvold, Genovese and Shimony (2024) for a deep theoretical and experimental discussion of Bell inequality violations. |
| 14 | An EPR-Bohm experiment with electrons consists in a setup in which a source of entangled electron pairs is situated between two analysers respectively located on the left and right wing of the array. The analysers are Stern-Gerlach apparatuses whose characteristic axes are determined by the directions of their magnetic fields that measure the spin component of the impinging electron. The pair of entangled electrons that travel in opposite directions from the source towards the analysers are generated in the spin-singlet state, i. e., the spin components of both electrons in each pair are anticorrelated for any considered direction in space (Baladrón and Khrennikov, 2019; Myrvold, Genovese and Shimony, 2024). |
| 15 | Parameter independence and outcome independence are the two conditions in which the so-called factorizability or Bell locality condition can be decomposed following Shimony’s terminology (Myrvold, Genovese and Shimony, 2024). This factorizability condition expresses the central explicit hypothesis in the Bell’s theorem (Myrvold, Genovese and Shimony, 2024). The Bell’s theorem contends that those theories satisfying the factorizability condition and certain additional conditions cannot reproduce the predictions of quantum mechanics under all circumstances. Assuming an EPR-Bohm experiment with pairs of entangled electrons in the spin singlet state and that the choice of the orientation of the analyser axis on one arm of the setup is made at spacelike separation from the other arm of the experiment, parameter independence asserts that the probability of obtaining a certain result on one arm of the EPR-Bell experiment for any orientation of the analyser’s axis does not depend on the orientation of the analyser’s axis on the other arm. Outcome independence expresses the condition that, for any couple of fixed orientations of the analysers’ axes on both sides of the setup, the probability of obtaining an outcome on one side of the experiment does not depend on the outcome on the other side. |
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