TY - JOUR
T1 - Effect of cation substitution on magnetic properties in Mn 1-xA'xCr2S4 (A' = Cd, Zn) thiospinel series
AU - Barahona, P.
AU - Galdamez, A.
AU - Manríquez, V.
AU - Cruzat, C.
AU - Raison, C.
AU - Le Coz, S.
AU - Peña, O.
AU - Moure, C.
PY - 2010/10
Y1 - 2010/10
N2 - Colossal magnetoresistance (CMR) materials such as REMnO3 perovskites and AB2S4 thiospinels have been well studied in the past. The authors present thiospinel compounds with A = Mn, since they may be viewed as a link to REMnO3 CMR perovskites. Ferrimagnetic MnCr2S4 is known to present a Tc of 65 K and a magnetic transition towards a non-collinear Yafet-Kittel state. The (Mn 1-xA'x)Cr2S4 series (A = Cd, Zn) was synthesised at 850°C. This series crystallises in the space group Fd3m with a close to 10 Å. When A' = Cd (Tc ranging from 68 K, x = 0·2, to 79 K, x = 0·6), the ferromagnetic features are enhanced, indicating that antiferromagnetism between Mn spins is progressively lost. For A' = Zn, two magnetic transitions take place, one at 15 K, which is reminiscent of the antiferromagnetic state of ZnCr2S4 and another one at Tc = 115 K. Impurities which could be responsible of these two magnetic states are excluded.
AB - Colossal magnetoresistance (CMR) materials such as REMnO3 perovskites and AB2S4 thiospinels have been well studied in the past. The authors present thiospinel compounds with A = Mn, since they may be viewed as a link to REMnO3 CMR perovskites. Ferrimagnetic MnCr2S4 is known to present a Tc of 65 K and a magnetic transition towards a non-collinear Yafet-Kittel state. The (Mn 1-xA'x)Cr2S4 series (A = Cd, Zn) was synthesised at 850°C. This series crystallises in the space group Fd3m with a close to 10 Å. When A' = Cd (Tc ranging from 68 K, x = 0·2, to 79 K, x = 0·6), the ferromagnetic features are enhanced, indicating that antiferromagnetism between Mn spins is progressively lost. For A' = Zn, two magnetic transitions take place, one at 15 K, which is reminiscent of the antiferromagnetic state of ZnCr2S4 and another one at Tc = 115 K. Impurities which could be responsible of these two magnetic states are excluded.
KW - Cooperative phenomena
KW - Ferrimagnetism
KW - Interacting sublattices
KW - Spin reorientation
UR - https://doi.org/10.36331/revista.v6i1.67
U2 - 10.1179/174367609X414125
DO - 10.1179/174367609X414125
M3 - Artículo
AN - SCOPUS:77957571601
SN - 1743-6753
VL - 109
SP - 431
EP - 435
JO - Advances in Applied Ceramics
JF - Advances in Applied Ceramics
IS - 7
ER -