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.
- 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