Abstract

Researchers propose a new ``many-interacting-worlds'' theory that could explain quantum mechanics in all its strangeness. Numerical simulations reproduce wave behavior in double-slit experiments assuming as few as 40 worlds.

Highlights

  • The role of the wave function differs markedly in various formulations of quantum mechanics

  • We investigate whether quantum theory can be understood as the continuum limit of a mechanical theory, in which there is a huge, but finite, number of classical “worlds,” and quantum effects arise solely from a universal interaction between these worlds, without reference to any wave function

  • We introduce a simple model of such a “many interacting worlds” approach and show that it can reproduce some generic quantum phenomena—such as Ehrenfest’s theorem, wave packet spreading, barrier tunneling, and zero-point energy—as a direct consequence of mutual repulsion between worlds

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Summary

INTRODUCTION

The role of the wave function differs markedly in various formulations of quantum mechanics. In Madelung’s quantum hydrodynamics [5], Nelson’s stochastic dynamics [6], and Hall and Reginatto’s exact uncertainty approach [7], the fundamental equations of motion are formulated in terms of a configuration probability density P and a momentum potential S (or the gradient of the latter), with a purely formal translation to a wave function description via Ψ ≔ P1=2 exp1⁄2iS=ħŠ. Regarded as a fundamental physical theory in its own right, the MIW approach may lead to new predictions arising from the restriction to a finite number of worlds It provides a natural discretization of the Holland-Poirier approach, which may be useful for numerical purposes. Before considering how its dynamics might be mathematically formulated and used as a numerical tool, we give a brief discussion of how its ontology may appeal to those who favor realist interpretations

Comparative ontology of the MIW approach
Outline of the paper
From dBB to MIW
Probabilities and the quantum limit
Which initial data give rise to quantum behavior?
Interworld interaction potential
SIMPLE EXAMPLE
One-dimensional toy model
Nðxnþ1
Basic properties of the toy model
QUANTUM PHENOMENA AS GENERIC MIW EFFECTS
Ehrenfest theorem
Wave packet spreading
N ðtÞ x2n
Barrier tunneling
Nonclassical transmission
Nonclassical reflection
Zero-point energy
Heisenberg-type uncertainty relation
SIMULATING QUANTUM GROUND STATES
Oscillator ground states
ÁÁÁ þ ξn ð42Þ subject to the constraints
SIMULATING QUANTUM EVOLUTION
CONCLUSIONS

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