Curie's principle and spontaneous symmetry breaking
International Studies in the Philosophy of Science 18 (2 & 3):173 – 198 (2004)
| Abstract | In 1894 Pierre Curie announced what has come to be known as Curie's Principle: the asymmetry of effects must be found in their causes. In the same publication Curie discussed a key feature of what later came to be known as spontaneous symmetry breaking: the phenomena generally do not exhibit the symmetries of the laws that govern them. Philosophers have long been interested in the meaning and status of Curie's Principle. Only comparatively recently have they begun to delve into the mysteries of spontaneous symmetry breaking. The present paper aims to advance the discussion of both of these twin topics by tracing their interaction in classical physics, ordinary quantum mechanics and quantum field theory. The features of spontaneous symmetry that are peculiar to quantum field theory have received scant attention in the philosophical literature. These features are highlighted here, along with an explanation of why Curie's Principle, though valid in quantum field theory, is nearly vacuous in that context. | |||||||||
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Chuang Liu (2003). Classical Spontaneous Symmetry Breaking. Philosophy of Science 70 (5):1219-1232.
Chuang Liu (2003). Spontaneous Symmetry Breaking and Chance in a Classical World. Philosophy of Science 70 (3):590-608.
Jenann Ismael (1997). Curie's Principle. Synthese 110 (2):167-190.
Alexandre Laforgue (1994). Les Brisures de Symetrie du Temps. Acta Biotheoretica 42 (1).
Alexandre Laforgue (1993). Les Brisures de Symetrie du Temps. Acta Biotheoretica 41 (1-2).
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