TY - JOUR
T1 - Doping-Dependent Magnetism and Exchange Bias in CaMn1-xRexO3
AU - Markovich, Vladimir
AU - Fita, Ivan
AU - Wisniewski, Andrzej
AU - Puzniak, Roman
AU - Martin, Christine
AU - Mogilyansky, Dmitrii
AU - Jung, Grzegorz
AU - Gorodetsky, Gad
N1 - Publisher Copyright:
© 1965-2012 IEEE.
PY - 2017/4/1
Y1 - 2017/4/1
N2 - Magnetic and structural properties of CaMn1-xRexO3 (0.02 ≤ x ≤ 0.1) have been investigated. Substitution of Re5+ ion for the Mn4+ site of 3 generates Mn3+ ions according to the chemical formula CaMn1-2x4+Mnx3+Rex5+O3, accompanied by an increase of lattice parameters and unit-cell volume with increasing {x}. With increasing doping level x , the magnetic ground state evolves from an antiferromagnetic (AFM) with a weak ferromagnetic (FM) component, for x = 0.02 - 0.06 , to the charge ordered {C} -type AFM state at x = 0.1. Spontaneous magnetization at T = 10 K increases quickly with increasing x , approaches the maximum value of 3.5 eμg for x = 0.04 , and then decreases rapidly to 0.2 eμg for x = 0.1. Anomalous negative magnetization (NM) for x = 0.02 has been observed in the zero-field-cooled and field-cooled (FC) magnetization below the magnetic transition temperature. Exchange bias (EB) effect, manifested by horizontal shift in the hysteresis loops of FC samples, has also been observed. This effect is very small for x = 0.02 , almost zeroes for 0.04, and monotonously increases with increasing x. The EB appears due to low-temperature phase separation into FM clusters and charge-ordered AFM phases. The effect of hydrostatic pressure for all samples revealed a significant increase of the FM phase volume under pressure, linked to both suppression of NM in x = 0.02 sample and reduction of the EB effect in all samples.
AB - Magnetic and structural properties of CaMn1-xRexO3 (0.02 ≤ x ≤ 0.1) have been investigated. Substitution of Re5+ ion for the Mn4+ site of 3 generates Mn3+ ions according to the chemical formula CaMn1-2x4+Mnx3+Rex5+O3, accompanied by an increase of lattice parameters and unit-cell volume with increasing {x}. With increasing doping level x , the magnetic ground state evolves from an antiferromagnetic (AFM) with a weak ferromagnetic (FM) component, for x = 0.02 - 0.06 , to the charge ordered {C} -type AFM state at x = 0.1. Spontaneous magnetization at T = 10 K increases quickly with increasing x , approaches the maximum value of 3.5 eμg for x = 0.04 , and then decreases rapidly to 0.2 eμg for x = 0.1. Anomalous negative magnetization (NM) for x = 0.02 has been observed in the zero-field-cooled and field-cooled (FC) magnetization below the magnetic transition temperature. Exchange bias (EB) effect, manifested by horizontal shift in the hysteresis loops of FC samples, has also been observed. This effect is very small for x = 0.02 , almost zeroes for 0.04, and monotonously increases with increasing x. The EB appears due to low-temperature phase separation into FM clusters and charge-ordered AFM phases. The effect of hydrostatic pressure for all samples revealed a significant increase of the FM phase volume under pressure, linked to both suppression of NM in x = 0.02 sample and reduction of the EB effect in all samples.
KW - Exchange bias (EB)
KW - hysteresis loop
KW - magnetization
KW - phase separation
UR - http://www.scopus.com/inward/record.url?scp=85016159823&partnerID=8YFLogxK
U2 - 10.1109/TMAG.2016.2626470
DO - 10.1109/TMAG.2016.2626470
M3 - Article
AN - SCOPUS:85016159823
SN - 0018-9464
VL - 53
JO - IEEE Transactions on Magnetics
JF - IEEE Transactions on Magnetics
IS - 4
M1 - 7738468
ER -