Goldstone modes: Difference between revisions
Jump to navigation
Jump to search
Carl McBride (talk | contribs) (New page: {{Stub-general}} '''Goldstone modes''' (also known as Goldstone bosons) arise from Goldstone's conjecture; that if there is continuous symmetry transformation under which the Lagrangian is...) |
Carl McBride (talk | contribs) m (Added a recent publication) |
||
| Line 1: | Line 1: | ||
{{Stub-general}} | {{Stub-general}} | ||
'''Goldstone modes''' (also known as Goldstone bosons) arise from Goldstone's conjecture; that if there is continuous symmetry transformation under which the Lagrangian is invariant, then either the vacuum state is also invariant under the transformation, or there must exist spinless particles of zero mass. | '''Goldstone modes''' (also known as Nambu-Goldstone bosons)<ref>[http://dx.doi.org/10.1103/PhysRev.122.345 Y. Nambu and G. Jona-Lasinio "Dynamical Model of Elementary Particles Based on an Analogy with Superconductivity. I", Physical Review '''122''' pp. 345-358 (1961)]</ref> | ||
<ref>[http://dx.doi.org/10.1103/PhysRev.127.965 Jeffrey Goldstone, Abdus Salam and Steven Weinberg "Broken Symmetries", Physical Review '''127''' pp. 965-970 (1962)]</ref> arise from Goldstone's conjecture; that if there is continuous symmetry transformation under which the Lagrangian is invariant, then either the vacuum state is also invariant under the transformation, or there must exist spinless particles of zero mass. | |||
==See also== | ==See also== | ||
*[[Mermin-Wagner theorem]] | *[[Mermin-Wagner theorem]] | ||
==References== | ==References== | ||
<references/> | |||
;Related reading | |||
*[http://dx.doi.org/10.1007/BF01646487 Sidney Coleman "There are no Goldstone bosons in two dimensions", Communications in Mathematical Physics '''31''' pp. 259-264 (1973)] | |||
*[http://dx.doi.org/10.1103/PhysRevLett.108.251602 Haruki Watanabe and Hitoshi Murayama "Unified Description of Nambu-Goldstone Bosons without Lorentz Invariance", Physical Review Letters '''108''' 251602 (2012)] | |||
[[category: quantum mechanics]] | |||
Latest revision as of 11:43, 25 June 2012
|
This article is a 'stub' page, it has no, or next to no, content. It is here at the moment to help form part of the structure of SklogWiki. If you add sufficient material to this article then please remove the {{Stub-general}} template from this page. |
Goldstone modes (also known as Nambu-Goldstone bosons)[1] [2] arise from Goldstone's conjecture; that if there is continuous symmetry transformation under which the Lagrangian is invariant, then either the vacuum state is also invariant under the transformation, or there must exist spinless particles of zero mass.
See also[edit]
References[edit]
- Related reading