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A Matter of Degree: Putting Unitary Inequivalence to Work

Published online by Cambridge University Press:  01 January 2022

Abstract

If a classical system has infinitely many degrees of freedom, its Hamiltonian quantization need not be unique up to unitary equivalence. I sketch different approaches (Hilbert space and algebraic) to understanding the content of quantum theories in light of this non-uniqueness, and suggest that neither approach suffices to support explanatory aspirations encountered in the thermodynamic limit of quantum statistical mechanics.

Type
Quantum Field Theory, Bell's Theorem, and Hidden Variables
Copyright
Copyright © The Philosophy of Science Association

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Footnotes

For comments on earlier drafts, I am obliged to Gordon Belot, Jeremy Butterfield, Rob Clifton, and John Earman.

References

Bratteli, Ola, and Robinson, Derek W. (1987), Operator Algebras and Quantum Statistical Mechanics 1, 2nd ed. Berlin: Springer-Verlag.CrossRefGoogle Scholar
Bratteli, Ola, and Robinson, Derek W. (1997), Operator Algebras and Quantum Statistical Mechanics 2, 2nd ed. Berlin: Springer-Verlag.CrossRefGoogle Scholar
Callender, Craig (2001), “Taking Thermodynamics Too Seriously”, Taking Thermodynamics Too Seriously 32:539554.Google Scholar
Clifton, Rob, and Halvorson, Hans (2001), “Are Rindler Quanta Real?”, Are Rindler Quanta Real? 52:417470.Google Scholar
Emch, Gerard G. (1984), Mathematical and Conceptual Foundations of Twentieth Century Physics. Amsterdam: North-Holland.Google Scholar
Emch, Gerard G., and Knops, H.J.F. (1970), “Pure thermodynamic phases as extremal KMS states”, Pure thermodynamic phases as extremal KMS states 11:30083018.Google Scholar
Kadison, Richard (1965), “Transformations of States in Operator Theory and Dynamics”, Transformations of States in Operator Theory and Dynamics 3, Suppl. 2:177198.Google Scholar
Haag, Rudolf (1962), “The Mathematical Structure of the Bardeen-Cooper-Schrieffer Model”, The Mathematical Structure of the Bardeen-Cooper-Schrieffer Model 25:287299.Google Scholar
Kronz, Fred, and Lupher, Tracy (2001), “Unitarily Inequivalent Representations in Algebraic Quantum Theory”, pre-print.Google Scholar
Primas, Hans (1983), Chemistry, Quantum Mechanics, and Reductionism. New York: Springer-Verlag.CrossRefGoogle Scholar
Robinson, Derek W. (1966), “Algebraic Aspects of Relativistic Quantum Field Theory”, in Chretien, M. and Deser, S. (eds.), Axiomatic Field Theory. New York: Gordon and Breach.Google Scholar
Ruelle, David (1969), Statistical Mechanics. New York: W.A. Benjamin.Google Scholar
Segal, Irving (1967), “Representation of Canonical Commutation Relations”, in Lurçat, François (ed.), Cargese Lectures in Theoretical Physics. New York: Gordon and Breach.Google Scholar
Sewell, Geoffrey L. (1986), Quantum Theory of Collective Phenomena. Oxford: Oxford University Press.Google Scholar
Wald, Robert M. (1994), Quantum Field Theory in Curved Spacetime and Black Hole Thermodynamics. Chicago: University of Chicago Press.Google Scholar