Both sides previous revision Previous revision Next revision | Previous revision | ||
advanced_tools:group_theory:conformal_group [2018/03/21 11:42] jakobadmin |
advanced_tools:group_theory:conformal_group [2018/05/27 13:52] (current) jakobadmin [Why is it interesting?] |
||
---|---|---|---|
Line 2: | Line 2: | ||
<tabbox Why is it interesting?> | <tabbox Why is it interesting?> | ||
+ | The maximal spacetime symmetry group of massless particles is the conformal group. | ||
+ | |||
+ | ---- | ||
Line 15: | Line 18: | ||
<cite>page 621 Einstein Gravity in a Nutshell - A. Zee</cite> | <cite>page 621 Einstein Gravity in a Nutshell - A. Zee</cite> | ||
</blockquote> | </blockquote> | ||
+ | |||
+ | <blockquote>"The simplest example of conformal matter is a perfect fluid of radiation. In the context of cosmology, this is extremely well motivated since the early Universe was, we believe, radiation dominated." <cite>https://arxiv.org/pdf/1612.02792.pdf</cite></blockquote> | ||
<tabbox Layman> | <tabbox Layman> | ||
Line 21: | Line 26: | ||
<tabbox Student> | <tabbox Student> | ||
- | <WRAP tip>The conformal group is $SO(4,2)$ or its double cover $SU(2,2)$ [[http://math.ucr.edu/home/baez/symmetries.html|Source]]</WRAP> | + | * The conformal group is $SO(4,2)$ or its double cover $SU(2,2)$ [[http://math.ucr.edu/home/baez/symmetries.html|Source]] |
- | + | * For a nice discussion, see [[http://aip.scitation.org/doi/pdf/10.1063/1.1665843|On Representations of the Conformal Group Which When Restricted to Its Poincare or Weyl Subgroups Remain Irreducible]] by J. Mickelsson | |
- | For a nice discussion, see [[http://aip.scitation.org/doi/pdf/10.1063/1.1665843|On Representations of the Conformal Group Which When Restricted to Its Poincare or Weyl Subgroups Remain Irreducible]] by J. Mickelsson | + | * For the definition of the group and the algebra, see [[https://books.google.de/books?id=H90XDQAAQBAJ&lpg=PA188&ots=5JxDa7kfpc&dq=%22su(2%2C2)%22%20Lie%20algebra&hl=de&pg=PA188#v=onepage&q&f=false|this chapter]]. |
- | + | * The conformal group is a subgroup of the diffeomorphism group. Under a conformal transformation, the metric changes as | |
- | "//the conformal algebra is equivalent to SO(2, 4), the algebra of rotations and boosts in a six dimensional | + | |
- | space with two time-like directions.//" http://homepages.uc.edu/~argyrepc/cu661-gr-SUSY/susy2001.pdf | + | |
- | + | ||
- | + | ||
- | For the definition of the group and the algebra, see [[https://books.google.de/books?id=H90XDQAAQBAJ&lpg=PA188&ots=5JxDa7kfpc&dq=%22su(2%2C2)%22%20Lie%20algebra&hl=de&pg=PA188#v=onepage&q&f=false|this chapter]]. | + | |
- | + | ||
- | The conformal group is a subgroup of the diffeomorphism group. Under a conformal transformation, the metric changes as | + | |
$$ g_{\mu\nu}\to \Omega(x)g_{\mu\nu} $$ | $$ g_{\mu\nu}\to \Omega(x)g_{\mu\nu} $$ | ||
or equivalently | or equivalently | ||
$$ d\tau \to \Omega(x) d\tau , $$ | $$ d\tau \to \Omega(x) d\tau , $$ | ||
where $\Omega(x) = \mathrm{e}^{i \omega(x)}$ is a scalar factor. | where $\Omega(x) = \mathrm{e}^{i \omega(x)}$ is a scalar factor. | ||
+ | |||
+ | <blockquote>"//the conformal algebra is equivalent to SO(2, 4), the algebra of rotations and boosts in a six dimensional | ||
+ | space with two time-like directions.//" http://homepages.uc.edu/~argyrepc/cu661-gr-SUSY/susy2001.pdf</blockquote> | ||
+ | |||
+ | |||
+ | |||