Symmetry breaking
Symmetry breaking in physics describes a phenomenon where (infinitesimally) small fluctuations acting on a system which is crossing a critical point decide the system's fate, by determining which branch of a bifurcation is taken. To an outside observer unaware of the fluctuations (or "noise"), the choice will appear arbitrary. This process is called symmetry "breaking", because such transitions usually bring the system from a disorderly state into one of two definite states. Symmetry breaking is supposed to play a major role in pattern formation.
In particular, we distinguish between:
- Explicit symmetry breaking where the laws describing a system are themselves not invariant under the symmetry in question.
- Spontaneous symmetry breaking where the laws are invariant but the system isn't because the background of the system, its vacuum, is non-invariant. Such a symmetry breaking is parametrized by an order parameter. A special case of this type of symmetry breaking is dynamical symmetry breaking.
In 1972, Nobel laureate P.W. Anderson used the idea of Symmetry breaking to show some of the drawbacks of Reductionism in his paper titled More is different in Science.[1]
One of the first cases of broken symmetry discussed in the physics literature is related to the form taken by a uniformly rotating body of incompressible fluid in gravitational and hydrostatical equilibrium. Jacobi[2] and soon later Liouville[3], in 1834, discussed the fact that an tri-axial ellipsoid was an equilibrium solution for this problem when the kinetic energy compared to the gravitational energy of the rotating body exceded a certain critical value. The axial symmetry presented by the McLaurin spheroids is broken at this bifurcation point. Furthermore, above this bifurcation point, and for constant angular momentum, the solution that minimizes the kinetic energy are the non-axially symmetric Jacobi ellipsoids instead of the Maclaurin spheroids.
[edit] See also
- Higgs mechanism
- QCD vacuum
- Goldstone boson
- 1964 PRL symmetry breaking papers
- J. J. Sakurai Prize for Theoretical Particle Physics
- Spontaneous symmetry breaking
[edit] References
- ^ Anderson, P.W. (1972). "More is Different". Science 177 (4047): 393–396. Bibcode 1972Sci...177..393A. doi:10.1126/science.177.4047.393. PMID 17796623. http://www.isnature.org/Files/Anderson_More_is_Different.pdf.
- ^ Jacobi, C.G.J. (1834). "Über die figur des gleichgewichts". Poggendorf Ann. Phys. Chim (33): 229–238.
- ^ Liouville, J. (1834). "Sur la figure d'une masse fluide homogène, en équilibre et douée d'un mouvement de rotation". Journal de l'École Polytechnique (14): 289-296.
