Crystal-Field Effects in the Tight-Binding Approximation: ReO3and Perovskite Structures

1970 ◽  
Vol 2 (10) ◽  
pp. 3918-3935 ◽  
Author(s):  
L. F. Mattheiss
1979 ◽  
Vol 40 (C5) ◽  
pp. C5-180-C5-182 ◽  
Author(s):  
J. X. Boucherle ◽  
D. Givord ◽  
J. Laforest ◽  
J. Schweizer ◽  
F. Tasset

1976 ◽  
Vol 18 (3) ◽  
pp. 303-306 ◽  
Author(s):  
S.G. Sankar ◽  
S.K. Malik ◽  
V.U.S. Rao

2005 ◽  
Vol 13 (1-3) ◽  
pp. 179-182 ◽  
Author(s):  
A.D. Christianson ◽  
J.M. Lawrence ◽  
P.S. Riseborough ◽  
N.O. Moreno ◽  
P.G. Pagliuso ◽  
...  
Keyword(s):  

2021 ◽  
Vol 197 ◽  
pp. 110678
Author(s):  
Daniele Barettin ◽  
Alessandro Pecchia ◽  
Matthias Auf der Maur ◽  
Aldo Di Carlo ◽  
Benny Lassen ◽  
...  

1985 ◽  
Vol 52 (1-4) ◽  
pp. 208-210 ◽  
Author(s):  
T. Okamoto ◽  
H. Fujii ◽  
Y. Andoh ◽  
H. Fujiwara

1989 ◽  
Vol 81 (3) ◽  
pp. 313-317 ◽  
Author(s):  
L. Iannarella ◽  
X.A. da Silva ◽  
A.P. Guimarães

2021 ◽  
pp. 2150286
Author(s):  
Erhan Albayrak

The outcome of the random crystal field effects on the antiferromagnetic spin-1 Blume–Capel model and external magnetic field are examined on the Bethe Lattice in terms of exact recursion relations. It is assumed that the crystal field is either turned on or off randomly with probability [Formula: see text] and [Formula: see text], respectively. The phase diagrams are constructed from the thermal analysis of the order parameters with the coordination number [Formula: see text] which corresponds to honeycomb lattice. It is explored that the system goes both second- and first-order phase transitions, along with the reentrant behavior and a few critical points. The reentrant behavior is stronger for lower values of [Formula: see text] and disappears as [Formula: see text] gets closer to 1.0. The first-order lines are observed to be either linked to the tricritical points or decomposed. The critical end points and double critical points are also observed.


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