Jump to content

Lambda transition

From Wikipedia, the free encyclopedia
This is an old revision of this page, as edited by Jack Greenmaven (talk | contribs) at 10:05, 29 November 2013 (Reverted 1 edit by 14.139.155.114 identified as test/vandalism using STiki). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.

The λ (lambda) universality class is probably the most important group in condensed matter physics. It regroups several systems possessing strong analogies, namely, superfluids, superconductors and smectics (liquid crystals). All these systems are expected to belong to the same universality class for the thermodynamic critical properties of the phase transition. While these systems are quite different at the first glance, they all are described by similar formalisms and their typical phase diagrams are identical.

See also

References

Books

  • Chaikin P. M. and Lubensky T. C. Principles of Condensed Matter Physics (Cambridge University Press, Cambridge) 1995, sect.9.
  • Feynman R. P. Progress in Low Temperature Physics Vol.1, edited by C. Gorter (North Holland, Amsterdam) 1955.

Journal articles

  • Helfrich W. J. Phys. (Paris) 39 (1978) 1199.
  • Nelson D. R. and Toner J. Phys. Rev. B 24 (1981) 363.
  • Dagupta C. and Halperin B. I. Phys. Rev. Lett.47 (1981) 1556.
  • Williams G. A. Phys. Rev. Lett. 59 (1987) 1926.
  • Onsager L. Nuovo Cimento Suppl. 6 (1949) 279.
  • de Gennes P.-G. Sol. State Commun. 10 (1972) 753.
  • Abrikosov A. A. Zh. Eksp. Teor. Fiz. 32 (1957) 1442.
  • Abrikosov A. A. Sov. Phys. JETP 5 (1957) 1174.
  • Renn S. and Lubensky T. C. Phys. Rev. A 38 (1988) 2132.