Systematic Trends in Short-Range Coulomb Effects among Nearly One-Dimensional Organic Conductors

1983 ◽  
Vol 50 (3) ◽  
pp. 207-211 ◽  
Author(s):  
S. Mazumdar ◽  
A. N. Bloch
1993 ◽  
Vol 3 (1) ◽  
pp. 171-201 ◽  
Author(s):  
P. Wzietek ◽  
F. Creuzet ◽  
C. Bourbonnais ◽  
D. Jérome ◽  
K. Bechgaard ◽  
...  

2007 ◽  
Vol 142 (3-4) ◽  
pp. 477-480
Author(s):  
Noriaki Matsunaga ◽  
Katutosi Hino ◽  
Takamichi Ohta ◽  
Katsumi Yamashita ◽  
Kazushige Nomura ◽  
...  

1999 ◽  
Vol 10 (06) ◽  
pp. 1025-1038 ◽  
Author(s):  
A. BENYOUSSEF ◽  
N. BOCCARA ◽  
H. CHAKIB ◽  
H. EZ-ZAHRAOUY

Lattice models describing the spatial spread of rabies among foxes are studied. In these models, the fox population is divided into three-species: susceptible (S), infected or incubating (I), and infectious or rabid (R). They are based on the fact that susceptible and incubating foxes are territorial while rabid foxes have lost their sense of direction and move erratically. Two different models are investigated: a one-dimensional coupled-map lattice model, and a two-dimensional automata network model. Both models take into account the short-range character of the infection process and the diffusive motion of rabid foxes. Numerical simulations show how the spatial distribution of rabies, and the speed of propagation of the epizootic front depend upon the carrying capacity of the environment and diffusion of rabid foxes out of their territory.


2001 ◽  
Vol 120 (1-3) ◽  
pp. 1069-1070 ◽  
Author(s):  
E.S. Choi ◽  
H.Y. Kang ◽  
Y.J. Jo ◽  
J. Yeom ◽  
W. Kang

1981 ◽  
Vol 42 (7) ◽  
pp. 991-1002 ◽  
Author(s):  
H.J. Schulz ◽  
D. Jérome ◽  
A. Mazaud ◽  
M. Ribault ◽  
K. Bechgaard

2005 ◽  
Vol 71 (7) ◽  
Author(s):  
M. Dressel ◽  
K. Petukhov ◽  
B. Salameh ◽  
P. Zornoza ◽  
T. Giamarchi

2002 ◽  
Vol 12 (9) ◽  
pp. 381-384
Author(s):  
N. Matsunaga ◽  
A. Ayari ◽  
P. Moncea ◽  
K. Yamashita ◽  
A. Ishikawa ◽  
...  

Magnetoresistance and Hall resistance measurements have been carried out in the FISDW phase of deuterated (TMTSF)2C1O4 for various cooling rates through the anion ordering temperature. The Hall resistance in the intermediate cooled state, observed a very stable quantum Hall state above 9.0 T for slowly cooled, shows a step-like change from the phase between 10 and 17 T to the phase between 20 and 25 T with hysteresis between 14 and 21 T. This result suggests that there is a new phase transition around 15 T in deuterated (TMTSF)4ClO4. A possible ground state of the FISDW phase of (TMTSF)2C1O4 for various cooling rates is discussed from the viewpoint of the peculiar SDW nesting vector stabilized by the dimerized gap due to anion ordering.


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