Quantum Many-Worlds Interpretation and Its Extensions to Decision Theory, Game Theory, and Economics
Quantum Many-Worlds Interpretation and Its Extensions to Decision Theory, Game Theory, and Economics
Abstract
This paper explores the quantum many-worlds interpretation (MWI) and its implications beyond fundamental physics, extending to decision theory, game theory, and economics. Starting from the foundational principles of MWI, we examine how observers interact with branching universes, analyze Newcomb’s paradox in both classical and quantum forms, and discuss applications in quantum game theory and quantum economics. By integrating quantum concepts like superposition, entanglement, and interference, we demonstrate how these ideas resolve classical paradoxes and offer novel frameworks for modeling complex systems. Mathematical formulations are presented using Unicode symbols for clarity.
1. Introduction
The many-worlds interpretation of quantum mechanics, proposed by Hugh Everett III in 1957, posits that the universe branches into multiple parallel realities during quantum measurements, avoiding the wave function collapse postulate. This framework has profound philosophical and practical implications, particularly in understanding decision-making under uncertainty.
In this paper, we synthesize discussions on MWI, observer roles in branching, Newcomb’s paradox, its quantum variant, quantum game theory, and quantum economics. These topics form a coherent progression from quantum foundations to applied interdisciplinary fields, highlighting how quantum principles can reshape classical theories.
2. Quantum Many-Worlds Interpretation
2.1 Core Principles
The state of a quantum system is described by the wave function Ψ, which evolves linearly according to the Schrödinger equation:
iℏ ∂/∂t Ψ = Ĥ Ψ
where Ĥ is the Hamiltonian operator, i is the imaginary unit, and ℏ is the reduced Planck’s constant.
In MWI, measurements do not collapse Ψ; instead, the universe splits into branches corresponding to each possible outcome. For a superposition state:
Ψ = α |up⟩ + β |down⟩
with |α|² + |β|² = 1, the measurement entangles the observer, resulting in:
Ψ = α |up, observer sees up⟩ + β |down, observer sees down⟩
Probabilities arise from the squared amplitudes |α|² and |β|², aligning with the Born rule.
2.2 Advantages and Challenges
MWI maintains mathematical consistency without ad hoc collapse. It resolves the measurement problem via decoherence, where environmental interactions make branches effectively independent. However, it faces criticisms for ontological extravagance (infinite universes) and unverifiability.
Decoherence is modeled by tracing out environmental degrees of freedom, leading to a reduced density matrix ρ that appears classical.
3. Observer’s Role in Branch Optimization
3.1 Limitations on Branch Selection
Observers cannot directly select branches, as branch weights are fixed by wave function amplitudes:
Ψ = α |A⟩ + β |B⟩, with weights |α|² and |β|².
Decisions themselves are quantum processes, branching accordingly.
3.2 Decision Theory in MWI
In the Deutsch-Wallace framework, rational agents maximize weighted utility across branches:
U_total = Σ_i |α_i|² U_i
This resolves paradoxes like Newcomb’s by equating strategies under certain conditions.
For quantum decision trees, strategies influence subsequent branch structures via measurements.
3.3 Applications
In quantum amplification, random number generators use superpositions like (1/√2)|0⟩ + (1/√2)|1⟩ to create balanced branches. Ethical implications redefine free will as shaping branch structures rather than outcomes.
4. Newcomb’s Paradox
4.1 Problem Setup
A predictor places contents in boxes A (fixed $1,000) and B (either $1,000,000 or $0 based on prediction). Choosing only B (one-boxing) yields ~$1,000,000 if predicted correctly; both (two-boxing) yields ~$1,000.
4.2 Conflicting Principles
Expected utility favors one-boxing:
For accuracy p ≈ 1, EU_one = p × 1,000,000 ≈ 1,000,000
EU_two = p × 1,000 + (1-p) × 1,001,000 ≈ 1,000
Dominance favors two-boxing, as it adds $1,000 regardless of B’s content.
4.3 Resolutions
Causal links or pre-commitment support one-boxing; coincidences support two-boxing. Philosophical ties to free will and determinism.
5. Quantum Newcomb’s Paradox
5.1 Quantum Setup
Boxes are entangled, e.g., |Ψ⟩ = (1/√2) (|0_A 1_B⟩ + |1_A 0_B⟩).
Player choice is a quantum operation; measurement collapses the state, ensuring correlation without retrocausality.
5.2 Mathematical Model
Using qubits, predictor applies Hadamard (H) and CNOT gates. Nash equilibria favor one-boxing analogs due to entanglement.
In extended models, quantum strategies achieve deterministic predictions.
5.3 Differences from Classical
Entanglement provides built-in correlation, invalidating dominance in some states.
6. Applications in Quantum Game Theory
6.1 Quantum Strategies
Strategies are unitary operators in SU(2). Initial entangled state:
|Ψ⟩ = cos(γ/2)|00⟩ + i sin(γ/2)|11⟩
Payoffs from Tr(ρ M), where ρ is the final density matrix.
6.2 Quantum Prisoner’s Dilemma
Classical Nash: (2,2); quantum: (3,3) via “magic” strategy U(θ=π/2, φ=0).
6.3 Broader Applications
In auctions, entanglement prevents collusion. In finance, quantum arbitrage uses entangled portfolios. Social applications include quantum voting and climate games.
7. Applications in Quantum Economics
7.1 Quantum Market Models
Prices as expectations: P(t) = ⟨ψ(t)| ˆP |ψ(t)⟩
Entangled assets: |Ψ_AB⟩ models non-local correlations.
7.2 Financial Tools
Quantum Monte Carlo for pricing: Z = ∫ D[path] exp(-S[path]/ℏ)
Risk: Quantum VaR via Tr[ρ ˆVaR(α)]
7.3 Macro and Micro Economics
Quantum multipliers: 1/(1 - ⟨MPC| ˆM |MPC⟩)
Consumer behavior via non-commuting utilities.
7.4 Empirical and Policy Implications
Quantum models explain market anomalies; applications in central banking and carbon markets.
8. Conclusion
MWI provides a unified framework for quantum phenomena, extending to resolve decision paradoxes and enhance game-theoretic and economic models. Quantum entanglement and superposition offer tools for modeling complexity, promising revolutions in interdisciplinary applications. Future work should focus on empirical validation and computational implementations.
References
This synthesis draws from foundational works by Everett (1957), Deutsch & Wallace (on decision theory), Nozick (1969) on Newcomb’s, Piotrowski & Sładkowski (2003) on quantum games, and Orrell & Haven on quantum economics.
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