How is spontaneous symmetry breaking possible? Understanding Wigner's theorem in light of unitary inequivalence

Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 44 (4):464-469 (2013)
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Abstract

We pose and resolve a puzzle about spontaneous symmetry breaking in the quantum theory of infinite systems. For a symmetry to be spontaneously broken, it must not be implementable by a unitary operator in a ground state's GNS representation. But Wigner's theorem guarantees that any symmetry's action on states is given by a unitary operator. How can this unitary operator fail to implement the symmetry in the GNS representation? We show how it is possible for a unitary operator of this sort to connect the folia of unitarily inequivalent representations. This result undermines interpretations of quantum theory that hold unitary equivalence to be necessary for physical equivalence.

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Author Profiles

Hans Halvorson
Princeton University
David Baker
University of Michigan, Ann Arbor

Citations of this work

On broken symmetries and classical systems.Benjamin Feintzeig - 2015 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 52 (Part B):267-273.

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References found in this work

Interpreting quantum field theory.Laura Ruetsche - 2002 - Philosophy of Science 69 (2):348-378.
Broken Symmetry and Spacetime.David John Baker - 2011 - Philosophy of Science 78 (1):128-148.
Explaining quantum spontaneous symmetry breaking.Chuang Liu & Gérard G. Emch - 2005 - Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics 36 (1):137-163.
Johnny’s So Long at the Ferromagnet.Laura Ruetsche - 2006 - Philosophy of Science 73 (5):473-486.

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