1980
DOI: 10.1016/0022-4596(80)90019-5
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Phase diagram and some physical properties of V2O3+x (0 ⩽ x ⩽ 0.080)

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Cited by 93 publications
(53 citation statements)
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“…2. The ZFC-FC hysteresis eect is seen from ∼ 50 to 145 K and magnetic transition from the AFM to PM state is seen at T t = 144 K. The value of T t is in line with those reported for the insulator-metal transition of V 2 O 3 powders (nanowires, nanocrystals), namely, if a light non-stoichiometry is considered [3,4]. Moreover, the magnetization curves observed at temperatures of T = 10300 K were linear and non-hysteretic.…”
Section: Methodssupporting
confidence: 75%
“…2. The ZFC-FC hysteresis eect is seen from ∼ 50 to 145 K and magnetic transition from the AFM to PM state is seen at T t = 144 K. The value of T t is in line with those reported for the insulator-metal transition of V 2 O 3 powders (nanowires, nanocrystals), namely, if a light non-stoichiometry is considered [3,4]. Moreover, the magnetization curves observed at temperatures of T = 10300 K were linear and non-hysteretic.…”
Section: Methodssupporting
confidence: 75%
“…It has been shown that the substitution of V by Ti stabilizes the metallic phase, while the insulating phase is supported by the other substitutes. [9][10][11] The stabilization of the metallic phase was explained by enhanced orbital overlap and band broadening, caused by the larger spatial extension of the Ti 3d orbitals with respect to the V states. 12 Since the orbitals of the other cations are more contracted, they form localized states in the V 3d conduction band that favor an insulating character of V 2 O 3 .…”
Section: Introductionmentioning
confidence: 99%
“…More recently, it was found that the metallic phase also undergoes an antiferromagnetic transition at low temperature [10,11] Single crystals of V203 were grown using a skull melter [12]. Thin plates were then annealed in a suitable CO-CO2 atmosphere at 1400 C for approximately 2 weeks to adjust the stoichiometry uniformly [13].…”
mentioning
confidence: 99%