TY - JOUR
T1 - Organic conductors and superconductors at high field
AU - Chaikin, P. M.
AU - Kang, W.
AU - Hannahs, S.
AU - Yu, R. C.
N1 - Funding Information:
This research was supported by the National Science Foundation under DMR 88-22532.
PY - 1992/3/2
Y1 - 1992/3/2
N2 - The organic charge transfer salts (TMTSF)2X (where X=ClO4, PF6, ReO4, etc.) are among the most remarkable materials discovered. A single crystal of the PF6 salt exhibits metallic, insulating, antiferromagnetic, spin density wave, and superconducting phases as well as quantum Hall effects (QHE) as temperature, pressure and magnetic field are varied. In addition there are new phenomena found in no other materials: a cascade of magnetic field induced transitions and a new form of quantum oscillations. The QHE is particularly interesting in that it is observed for the first time in a bulk crystal. Unlike the conventional integer effect which arises from noninteracting particles and some disorder, in these salts the QHE is the result of a collective spin density wave distortion which assures that the Fermi energy is always in the gap between Landau bands and the QHE steps are accompanied by first order phase transitions.
AB - The organic charge transfer salts (TMTSF)2X (where X=ClO4, PF6, ReO4, etc.) are among the most remarkable materials discovered. A single crystal of the PF6 salt exhibits metallic, insulating, antiferromagnetic, spin density wave, and superconducting phases as well as quantum Hall effects (QHE) as temperature, pressure and magnetic field are varied. In addition there are new phenomena found in no other materials: a cascade of magnetic field induced transitions and a new form of quantum oscillations. The QHE is particularly interesting in that it is observed for the first time in a bulk crystal. Unlike the conventional integer effect which arises from noninteracting particles and some disorder, in these salts the QHE is the result of a collective spin density wave distortion which assures that the Fermi energy is always in the gap between Landau bands and the QHE steps are accompanied by first order phase transitions.
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U2 - 10.1016/0921-4526(92)90128-F
DO - 10.1016/0921-4526(92)90128-F
M3 - Article
AN - SCOPUS:0027108431
SN - 0921-4526
VL - 177
SP - 353
EP - 360
JO - Physica B: Physics of Condensed Matter
JF - Physica B: Physics of Condensed Matter
IS - 1-4
ER -