© 2004 by British Society for the Philosophy of Science
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Quantum Selections, Propensities and the Problem of Measurement
Departamento de Lógica y Filosofía de la Ciencia, Facultad de Filosofía B, Universidad Complutense de Madrid, 28040 Madrid, Spain, msuarez{at}filos.ucm.es
This paper expands on, and provides a qualified defence of, Arthur Fine's selective interactions solution to the measurement problem. Fine's approach must be understood against the background of the insolubility proof of the quantum measurement. I first defend the proof as an appropriate formal representation of the quantum measurement problem. The nature of selective interactions, and more generally selections, is then clarified, and three arguments in their favour are offered. First, selections provide the only known solution to the measurement problem that does not relinquish any of the explicit premises of the insolubility proofs. Second, unlike some no-collapse interpretations of quantum mechanics, selections suffer no difficulties with non-ideal measurements. Third, unlike most collapse interpretations, selections can be independently motivated by an appeal to quantum propensities.
- Introduction
- The problem of quantum measurement
- 2.1 The ignorance interpretation of mixtures
- 2.2 The eigenstateeigenvalue link
- 2.3 The quantum theory of measurement
- 2.2 The eigenstateeigenvalue link
- 2.1 The ignorance interpretation of mixtures
- The insolubility proof of the quantum measurement
- 3.1 Some notation
- 3.2 The transfer of probability condition (TPC)
- 3.3 The occurrence of outcomes condition (OOC)
- 3.2 The transfer of probability condition (TPC)
- 3.1 Some notation
- A defence of the insolubility proof
- 4.1 Stein's critique
- 4.2 Ignorance is not required
- 4.3 The problem of quantum measurement is an idealisation
- 4.2 Ignorance is not required
- 4.1 Stein's critique
- Selections
- 5.1 Representing dispositional properties
- 5.2 Selections solve the measurement problem
- 5.3 Selections and ignorance
- 5.2 Selections solve the measurement problem
- 5.1 Representing dispositional properties
- Non-ideal selections
- 6.1 No-collapse interpretations and non-ideal measurements
- 6.2 Exact and approximate measurements
- 6.3 Selections for non-ideal interactions
- 6.4 Approximate selections
- 6.5 Implications for ignorance
- 6.2 Exact and approximate measurements
- 6.1 No-collapse interpretations and non-ideal measurements
- Selective interactions test quantum propensities
- 7.1 Equivalence classes as physical aspects: a critique
- 7.2 Quantum dispositions
- 7.3 Selections as a propensity modal interpretation
- 7.4 A comparison with Popper's propensity interpretation
- 7.2 Quantum dispositions
- 7.1 Equivalence classes as physical aspects: a critique