Editing Goldstone modes
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'''Goldstone modes''' (also known as | '''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. | ||
==See also== | ==See also== | ||
*[[Mermin-Wagner theorem]] | *[[Mermin-Wagner theorem]] | ||
==References== | ==References== | ||
#[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''' 345-358 (1961)] | |||
#[http://dx.doi.org/10.1103/PhysRev.127.965 Jeffrey Goldstone, Abdus Salam and Steven Weinberg "Broken Symmetries", Physical Review '''127''' 965-970 (1962)] | |||
#[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)] | |||
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