Symmetry: Difference between revisions

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Symmetries are intimately related to [[conservation law]]s via [[Noether's theorem]].
Symmetries are intimately related to [[conservation law]]s via [[Noether's theorem]].
== List of symmetries ==
Note that any given equation will typically only enjoy a subset of the symmetries on this list.
* [[Conformal]] symmetry
* [[Diffeomorphism symmetry]]
* [[Galilean]] symmetry
* [[Gauge]] invariance
* [[Lorentz]] symmetry
* [[Phase rotation symmetry]]
* [[Pseudoconformal]] symmetry
* [[Scaling]] symmetry
* [[Space rotation symmetry]]
* [[Space translation symmetry]]
* [[Time reversal symmetry]]
* [[Time translation symmetry]]


[[Category:Transforms]]
[[Category:Transforms]]

Revision as of 17:21, 15 August 2006


A symmetry of an equation is any operation which maps solutions to solutions; thus a symmetry is the same concept as a transform, except that the transformed equation is the same as the old.

In principle there are an infinite-dimensional space of symmetries; in practice, however, one works only with the finite-dimensional component of symmetries which have a clean and explicit algebraic description. Indeed many symmetries are linear in nature. Note that completely integrable equations enjoy an explicit infinite-dimensional space of symmetries, formed by using any of the infinite number of conserved quantities as a Hamiltonian.

The space of all symmetries form a group.

Symmetries are intimately related to conservation laws via Noether's theorem.

List of symmetries

Note that any given equation will typically only enjoy a subset of the symmetries on this list.