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Transcript
École Doctorale de Physique de la Région Parisienne
ED 107
Page Web : www.phys.ens.fr/Ecole.Doctorale/
COURS D’ÉCOLE DOCTORALE
QUANTUM CRITICALITY AND
HIGH-TEMPERATURE SUPERCONDUCTIVITY
Konstantin EFETOV, IPhT, Chaire Blaise Pascal & Bochum U.
Cours les vendredis 13, 20 et 27 Septembre, 04 et 11 Octobre 2013 à 10h
Institut de Physique Théorique
Salle Itzykson, Bât. 774 – Orme des Merisiers
In these lectures we discuss the behavior of a physical system near a quantum critical point
separating different phases. The word “quantum” reflects the fact that the transition occurs
also at zero temperature, with tuning parameters (like doping) characterizing the system.
For quite a long time it was assumed that quantum critical behavior in d dimensions is
similar to classical critical behavior in d+1 dimensions, where the extra dimension is time.
This makes it possible either to obtain scaling relations and calculate critical exponents, or to
conclude that the transition is of the first order.
Unexpectedly, a completely different scenario has been discovered recently in 2+1
dimensional models of fermions interacting with critical spin waves near a quantum
antiferromagnet-normal metal transition. Near such a quantum phase transition the system
develops an SU(2) order parameter, which characterizes the mixture of superconductivity
with a charge density wave. The resulting states, which completely differ from the original
antiferromagnetic state, are described by a non-linear sigma model and can be studied using
the renormalization group. In particular, at low temperature, the system can exhibit d-wave
superconductivity. Accumulating experimental evidence suggests that this scenario may well
describe the physics of high temperature superconducting cuprates.
The lectures will begin with the introduction of the concept of quantum criticality. It will
then be demonstrated how the symmetry is spontaneously broken, and why gapless
fluctuations are described by the SU(2) non-linear sigma model. Renormalization group
equations will be derived, leading to the phase diagram. Finally, the relevance of these ideas
to high temperature superconductivity in cuprates will be explained.
Renseignements : http://ipht.cea.fr
ou
[email protected]