Angular dependent magnetotransport and electronic structure in quasi-one-dimensional organic conductor (TMTSF)2ClO4

2001 ◽  
Vol 120 (1-3) ◽  
pp. 1029-1030 ◽  
Author(s):  
Kaya Kobayashi ◽  
Toshihito Osada
2001 ◽  
Vol 114-116 ◽  
pp. 717-721 ◽  
Author(s):  
M. Sing ◽  
R. Claessen ◽  
Th. Finteis ◽  
S. Hao ◽  
S. Hüfner ◽  
...  

2003 ◽  
Vol 68 (12) ◽  
Author(s):  
M. Sing ◽  
U. Schwingenschlögl ◽  
R. Claessen ◽  
P. Blaha ◽  
J. M. P. Carmelo ◽  
...  

Author(s):  
J. Fink

Conducting polymers comprises a new class of materials achieving electrical conductivities which rival those of the best metals. The parent compounds (conjugated polymers) are quasi-one-dimensional semiconductors. These polymers can be doped by electron acceptors or electron donors. The prototype of these materials is polyacetylene (PA). There are various other conjugated polymers such as polyparaphenylene, polyphenylenevinylene, polypoyrrole or polythiophene. The doped systems, i.e. the conducting polymers, have intersting potential technological applications such as replacement of conventional metals in electronic shielding and antistatic equipment, rechargable batteries, and flexible light emitting diodes.Although these systems have been investigated almost 20 years, the electronic structure of the doped metallic systems is not clear and even the reason for the gap in undoped semiconducting systems is under discussion.


2021 ◽  
Vol 103 (15) ◽  
Author(s):  
Olga Iakutkina ◽  
Lena Nadine Majer ◽  
Guilherme Gorgen Lesseux ◽  
Gabriele Untereiner ◽  
Martin Dressel

2004 ◽  
Vol 69 (3) ◽  
Author(s):  
S. Mitrovic ◽  
L. Perfetti ◽  
C. Søndergaard ◽  
G. Margaritondo ◽  
M. Grioni ◽  
...  

2015 ◽  
Vol 91 (23) ◽  
Author(s):  
Thomas E. Baker ◽  
E. Miles Stoudenmire ◽  
Lucas O. Wagner ◽  
Kieron Burke ◽  
Steven R. White

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.


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