Phenomenological Free-Energy Density Describing the Spin-Density-Wave State of Chromium

1980 ◽  
Vol 44 (19) ◽  
pp. 1261-1263 ◽  
Author(s):  
M. B. Walker
1995 ◽  
Vol 51 (13) ◽  
pp. 8347-8356 ◽  
Author(s):  
J. L. Musfeldt ◽  
M. Poirier ◽  
P. Batail ◽  
C. Lenoir

1995 ◽  
Vol 52 (22) ◽  
pp. 15983-15991 ◽  
Author(s):  
J. L. Musfeldt ◽  
M. Poirier ◽  
P. Batail ◽  
C. Lenoir

1993 ◽  
Vol 07 (19) ◽  
pp. 3415-3421 ◽  
Author(s):  
ALEXANDRE S. ROZHAVSKY

A field description of spin-density-wave (SDW) in a quasi-two-dimensional metal with open Fermi surface in magnetic field, is proposed. The SDW transition temperature, T c (H), and the Hall conductivity σxy, are calculated. The dependence T c (H) is found to be different from that of the Bardeen-Cooper-Schrieffer model, in particular, a threshold field, H c , found its natural explanation. It is proved that the quantized Hall conductivity arises from the chiral anomaly terms in the effective action provided there is pinning of chemical potential in the gap of extended states.


2002 ◽  
Vol 12 (9) ◽  
pp. 61-64
Author(s):  
C. Pasquier ◽  
M. Héritier ◽  
D. Jérome

We present a model comparing the free energy of a phase exhibiting a segregation between spin density wave (SDW) and metallic domains (eventually superconducting domains) and the free energy of homogeneous phases which explains the findings observed recently in (TMTSF)2PF6. The dispersion relation of this quasi-one-dimensional organic conductor is linearized around the Fermi level. Deviations from perfect nesting which stabilizes the SDW state are described by a unique parameter t$'_b$, this parameter can be the pressure as well.


1997 ◽  
Vol 56 (5) ◽  
pp. 2585-2593 ◽  
Author(s):  
S. Valfells ◽  
P. Kuhns ◽  
A. Kleinhammes ◽  
J. S. Brooks ◽  
W. Moulton ◽  
...  

1982 ◽  
Vol 25 (6A) ◽  
pp. 893-895 ◽  
Author(s):  
L Hedman ◽  
A Kjerulf ◽  
K V Rao ◽  
K Svensson ◽  
H U Åström

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