Antiparallel state, compensation point, and magnetic phase diagram of Fe3O4/Mn3O4 superlattices - art. no. 094421

Citation
G. Chern et al., Antiparallel state, compensation point, and magnetic phase diagram of Fe3O4/Mn3O4 superlattices - art. no. 094421, PHYS REV B, 6309(9), 2001, pp. 4421
Citations number
21
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B
ISSN journal
01631829 → ACNP
Volume
6309
Issue
9
Year of publication
2001
Database
ISI
SICI code
0163-1829(20010301)6309:9<4421:ASCPAM>2.0.ZU;2-Y
Abstract
The magnetic response of a ferrimagnetic/ferrimagnetic superlattice, [Fe3O4 (20 Angstrom)/Mn3O4 (80 Angstrom)](x20), is measured as a function of exte rnal field (-50-50 kOe) and temperature (5-300 K). A compensation point (T- cp) is identified similar to 33 K at which the remanence changes sign and l ow-field M-T curves show minima, indicating that the net moments of Fe3O4 a nd Mn3O4 are antiparallel. At temperatures >similar to 50 K, the magnetic r esponse becomes pure Fe3O4-like. Detailed M-H curves (at T<50 K) further ex hibit magnetic phase transition at higher external field. As H is above H*< similar to>10 kOe, the magnetization is enhanced and then saturates at H si milar to 40 kOe. These phases are similar to the twisted phases, originatin g from a competition between Zeeman and exchange energies, previously obser ved in antiparallel metallic multilayers. A H-T magnetic phase diagram of t he present superlattice is presented and five phases are included: the Mn3O 4-aligned, Fe3O4-aligned, twisted, ferrimagnetic saturated, and pure Fe3O4 phases; M-H curves also show asymmetry at temperatures below and above T-cp , which is probably related to the anisotropy effect of Mn3O4 (tetragonal s tructure). The fundamental mechanism of the antiparallel coupling between M n3O4 and Fe3O4 is also discussed.