Numéro |
J. Phys. IV France
Volume 131, December 2005
|
|
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Page(s) | 81 - 82 | |
DOI | https://doi.org/10.1051/jp4:2005131018 | |
Publié en ligne | 18 janvier 2006 |
S. Brazovskii, P. Monceau and N. Kirova
J. Phys. IV France 131 (2005) 81-82
DOI: 10.1051/jp4:2005131018
The ordered limit of superconductivity
V. Cvetkovic1, J. Zaanen2, 1, Z. Nussinov3 and S. Mukhin41 Instituut Lorentz voor de theoretische natuurkunde, Universiteit Leiden, PO Box 9506, NL-2300 RA Leiden, The Netherlands
2 Department of Physics, Stanford University, CA 94305, USA
3 Department of Physics, Washington University, St. Louis, MO 63160-4899, USA
4 Theoretical Physics Department, Moscow Institute for Steel and Alloys, 119991 Moscow, Russia
Abstract
The conventional understanding of superconductivity
rests heavily on the physics of Bose gases.
In the high temperature superconductors, the superfluid
is very strongly correlated being on the verge of solidifying into
a stripe phase. Inspired by this problem, we employ
quantum field theory techniques to construct the limit of "optimally
ordered"
superconductivity. These superconductors can be viewed as quantum
elastic
entities different from normal crystals in the sense that they
lost their rigidity against shear stress as dual Bose condensates of
quantum dislocations. Exciting new physical properties emerge
which can, in principle, be measured although they
invoke unconventional experiments: quantum liquid crystalline
orders, oscillations of magnetic screening currents, and
new collective modes found in the dynamical electromagnetic
response.
© EDP Sciences 2005