Abstract

Contemporary non-representationalist interpretations of the quantum state (especially QBism, neo-Copenhagen views, and the relational interpretation) maintain that quantum states codify observer-relative information. This paper provides an extensive defense of such views, while emphasizing the advantages of, specifically, the relational interpretation. The argument proceeds in three steps: (1) I present a classical example (which exemplifies the spirit of the relational interpretation) to illustrate why some of the most persistent charges against non-representationalism have been misguided. (2) The special focus is placed on dynamical evolution. Non-representationalists often motivate their views by interpreting the collapse postulate as the quantum mechanical analogue of Bayesian probability updating. However, it is not clear whether one can also interpret the Schrödinger equation as a form of rational opinion updating. Using results due to Hughes & van Fraassen as well as Lisi, I argue that unitary evolution has a counterpart in classical probability theory: in both cases (quantum and classical) probabilities relative to a non-participating observer evolve according to an entropy maximizing principle (and can be interpreted as rational opinion updating). (3) Relying on a thought-experiment by Frauchiger and Renner, I discuss the differences between quantum and classical probability models.

Highlights

  • The idea that quantum states do not represent physical reality is as old as quantum theory itself

  • Using results due to Hughes & van Fraassen as well as Lisi, I argue that unitary evolution has a counterpart in classical probability theory: in both cases probabilities relative to a non-participating observer evolve according to an entropy maximizing principle

  • [12] In other words, on the relational interpretation, quantum theory is interpreted along the following lines: from the previous point, we know that quantum state ascriptions are the result of preparation procedures, in which a correlation between measurement apparatus and system has been established. [11] At the same time, the point of collecting information in this way is that this allows predictions to be made for the outcomes of possible future interaction with other systems

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Summary

Introduction

The idea that quantum states do not represent (or correspond to) physical reality is as old as quantum theory itself. To see why dynamics would play an important role for non-representationalists, notice, first, that an important consequence of their shared commitment to observer-relative states is that the textbook dynamical postulates—von Neumann’s [17] collapse postulate and the unitary evolution of the Schrödinger equation—are not to be understood in terms of a mechanical/substance-type story of some entity collapsing or evolving Instead, those changes in the quantum state are to be understood as the process in which the observer rationally updates her opinion—either literally (QBism, neo-Copenhagen), or at least “on the model of” (relational interpretation).

I will make explicit how the set-up presented in the
The Basic Set-Up
Measurements
States
Betting-States
Odds Comparison
Number-States
Dynamics
How the Situation Looks from B’s Perspective
Preliminary Discussion—Some Advantages of the Example
The Betting-States are not “Absolute Descriptions”
Betting-States are Correlations
Completeness
Number-States are Expectation Values
Number-States are Coordinatizations
Treating O’s State as Privileged
Treating P’s State as Privileged
Argument from Interference
Argument from Scientific Realism
The Quantum State Is Not Epistemic!
Measurement Outcomes Are Not Objective!
Conclusions
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