TY - JOUR
T1 - Examining the oxygen isotope and magnetic field effect on phase separation in Sm0.5Sr0.5MnO3
AU - Styka, A. N.
AU - Ren, Y.
AU - Gorbenko, O. Yu
AU - Babushkina, N. A.
AU - Brown, D. E.
N1 - Publication details (e.g. title, author(s), publication statuses and dates) are captured on an “AS IS” and “AS AVAILABLE” basis at the time of record harvesting from the data source. Suggestions for further amendments or supplementary information can be sent to [email protected].
PY - 2006
Y1 - 2006
N2 - Magnetic field (MF) dependence of the phase separation (PS) in the manganites Sm0.5 Sr0.5 MnO3 with O 16 and O 18 was studied using high-resolution high-energy x-ray powder diffraction in the temperature range from 4.2 to 240 K and with the MF up to 6 T. Although the two compounds have an identical structure [a paramagnetic (PM) phase with the Pbnm symmetry] at room temperature, they show a significant difference in the PS region below Tps ∼110 K, where the O 16 sample has a structural inhomogeneity in the form of two coexisting ferromagnetic (FM) and antiferromagnetic (AF) phases, while the O 18 -sample phase separates into mixed AF and PM phases. The O 16 → O 18 isotope substitution appears to prevent the formation of the FM phase at low temperature. The application of a magnetic field significantly enhances the FM phase by converting other phases, leading to a homogeneous structure. The effects on the microscopic structure of the oxygen isotope substitution and external magnetic field play the key role in the physics behind the colossal magnetoresistance effect. © 2006 American Institute of Physics.
AB - Magnetic field (MF) dependence of the phase separation (PS) in the manganites Sm0.5 Sr0.5 MnO3 with O 16 and O 18 was studied using high-resolution high-energy x-ray powder diffraction in the temperature range from 4.2 to 240 K and with the MF up to 6 T. Although the two compounds have an identical structure [a paramagnetic (PM) phase with the Pbnm symmetry] at room temperature, they show a significant difference in the PS region below Tps ∼110 K, where the O 16 sample has a structural inhomogeneity in the form of two coexisting ferromagnetic (FM) and antiferromagnetic (AF) phases, while the O 18 -sample phase separates into mixed AF and PM phases. The O 16 → O 18 isotope substitution appears to prevent the formation of the FM phase at low temperature. The application of a magnetic field significantly enhances the FM phase by converting other phases, leading to a homogeneous structure. The effects on the microscopic structure of the oxygen isotope substitution and external magnetic field play the key role in the physics behind the colossal magnetoresistance effect. © 2006 American Institute of Physics.
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U2 - 10.1063/1.2375011
DO - 10.1063/1.2375011
M3 - RGC 21 - Publication in refereed journal
SN - 0021-8979
VL - 100
JO - Journal of Applied Physics
JF - Journal of Applied Physics
IS - 10
M1 - 103520
ER -