Source-linked AI summary

Distinct Quantum States Can Be Compatible with a Single State of Reality

Peter G. Lewis, David Jennings, Jonathan Barrett, Terry Rudolph

arXiv:1201.6554v2quant-ph

TL;DR

The paper asks whether distinct quantum states can correspond to overlapping distributions over underlying physical states, challenging a no-go result that assumes preparation independence. By explicitly constructing such models while retaining quantum predictions, it shows that ruling out ψ-epistemic models requires additional assumptions, although the constructions are contrived and do not meet the stronger overlap condition for every pair of non-orthogonal states.

  • Problem

    The paper asks whether quantum states can fail to uniquely determine underlying physical states, despite a no-go theorem based on preparation independence.

    Source: p. 1
  • Method

    The authors construct ontological models in which measurement outcomes depend on underlying states while distinct quantum-state distributions overlap.

    Source: pp. 2–3
  • Results

    Explicit constructions reproduce all quantum predictions while allowing ψ-epistemic overlap when preparation independence is abandoned.

    Source: pp. 1, 4
  • Takeaways & Limitations

    The result shows that any no-go theorem excluding ψ-epistemic models must use non-trivial assumptions beyond those required for a well-formed ontological model.

    Source: p. 1

    The models are contrived and do not have non-zero overlap for every pair of non-orthogonal quantum states.

    Source: p. 4

Abstract

from arXiv · show

Perhaps the quantum state represents information about reality, and not reality directly. Wave function collapse is then possibly no more mysterious than a Bayesian update of a probability distribution given new data. We consider models for quantum systems with measurement outcomes determined by an underlying physical state of the system but where several quantum states are consistent with a single underlying state---i.e., probability distributions for distinct quantum states overlap. Significantly, we demonstrate by example that additional assumptions are always necessary to rule out such a model.

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