scholarly journals Orbital disordering and the metal-insulator transition with hole doping in perovskite-type vanadium oxides

2005 ◽  
Vol 72 (2) ◽  
Author(s):  
J. Fujioka ◽  
S. Miyasaka ◽  
Y. Tokura
2018 ◽  
Vol 87 (2) ◽  
pp. 024708
Author(s):  
Shintaro Yamamoto ◽  
Daiki Ootsuki ◽  
Daiya Shimonaka ◽  
Daisuke Shibata ◽  
Kenjiro Kodera ◽  
...  

1997 ◽  
Vol 237-238 ◽  
pp. 6-10 ◽  
Author(s):  
Y. Tomioka ◽  
A. Asamitsu ◽  
H. Kuwahara ◽  
Y. Moritomo ◽  
M. Kasai ◽  
...  

2006 ◽  
Vol 243 (8) ◽  
pp. 1813-1822 ◽  
Author(s):  
M. Hidaka ◽  
M. Soejima ◽  
R. P. Wijesundera ◽  
M. Soda ◽  
M. Sato ◽  
...  

1998 ◽  
Vol 547 ◽  
Author(s):  
Hideki Taguchi

AbstractOrthorhombic perovskite-type (La0.1Ca0.9)(Mn1-xCox)O3 was synthesized in the range 0.00 ≤ x ≤ 0.08. The Rietveld analysis indicates that the (Mn, Co)-O(1 and 2) distances are independent of the composition (x). Measurements of the electrical resistivity (ρ) and the Seebeck coefficient (α) indicate that (La0.1Ca0.9)(Mn1-xCox)O3 is an n-type semiconductor at the low temperature. At the high temperature, (La0.1Ca0.9)(Mn1-xCox)O3 exhibits a metal-insulator transition in the range 0.0 ≤ x ≤ 0.04. The metal-insulator transition temperature (Tt) increases with increasing the Co3+ ion content, while dρ/dT in the metallic region decreases with increasing the Co3+ ion content. The variation of Ea and T+ is explained by the difference in the electronegativity between Mn and Co atoms. The variation of dρ/dT in the metallic region is explained by the increase in the collective o bond.


2015 ◽  
Vol 91 (20) ◽  
Author(s):  
Juan Gabriel Ramirez ◽  
Thomas Saerbeck ◽  
Siming Wang ◽  
J. Trastoy ◽  
M. Malnou ◽  
...  

2013 ◽  
Vol 2013 ◽  
pp. 1-6 ◽  
Author(s):  
A. L. Pergament ◽  
G. B. Stefanovich ◽  
N. A. Kuldin ◽  
A. A. Velichko

The problem of metal-insulator transition is considered. It is shown that the Mott criterion aB(nc)1/3≈0.25 is applicable not only to heavily doped semiconductors but also to many other materials, including some transition-metal compounds, such as vanadium oxides (particularly, VO2 and V2O3). The low-temperature transition (“paramagnetic metal—antiferromagnetic insulator”) in vanadium sesquioxide is described on the basis of this concept in terms of an intervening phase, between metal and insulator states, with divergent dielectric constant and effective charge carrier mass. Recent communications concerning a possible “metal-insulator transition” in vanadium pentoxide are also discussed.


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