MAGNETIC-PROPERTIES OF THE DILUTED FERRIMAGNET LI0.5FE1.1GA1.4O4 WITHSPATIALLY NONUNIFORM EXCHANGE

Citation
Nn. Efimova et Mb. Ustimenkova, MAGNETIC-PROPERTIES OF THE DILUTED FERRIMAGNET LI0.5FE1.1GA1.4O4 WITHSPATIALLY NONUNIFORM EXCHANGE, Journal of magnetism and magnetic materials, 185(3), 1998, pp. 360-368
Citations number
15
Categorie Soggetti
Material Science","Physics, Condensed Matter
ISSN journal
03048853
Volume
185
Issue
3
Year of publication
1998
Pages
360 - 368
Database
ISI
SICI code
0304-8853(1998)185:3<360:MOTDFL>2.0.ZU;2-6
Abstract
The isotherms of the specific magnetization, sigma(T)(H), and temperat ure dependences of the initial susceptibility, chi(o)(T), have been in vestigated in the temperature interval 77-300 It and in magnetic field s from 0 to 17 kOe as well as at T = 4.2 K and H less than or equal to 40 kOe on the diluted ferrimagnet. Li0.5Fe1.1Ga1.4O4. In this specime n, there is a spatial nonuniformity of the short-range indirect exchan ge interaction Fe3+-O-2-Fe3+ due to the composition disorder of nonmag netic ions Ga3+ in the spinel lattice. In order to change the extent a nd/or the character of this disorder, we used different regimes of hea r treating of the initially synthesized polycrystalline samples at 155 0 K: the quenching in air from T = 1550 IC (the Q sample) and the slow cooling to the room temperature together with the furnace (the SC sam ple). As a result of quenching an increase in the Curie point. T-c, fr om similar to 160 K (SC) to 240 K (Q) is observed, while the isotherm behaviour at 4.7 K differs only slightly (by similar to 5% in magnitud e of sigma). For the Q sample at T greater than or equal to 77 K irreg ular curves sigma(T)(H) are observed and the magnetization relaxation follows an exponential (T = 77 It, H = 0.71 kOe) or logarithmic law (T = 123 K, H = 0.74 kOe; T = 177 K, H = 0.73 kOe; T = 77 K, H = 1.55 kO e). Magnetic properties, the effects induced by the sample quenching i ncluded. are discussed within the model of the spatially nonuniform ma gnetic structure which may be visualized as two exchange-interacting s ubsystems: the matrix with a hi,eh concentration of the frustrated exc hange bonds and the clusters, where spins are coupled by a strong exch ange. (C) 1998 Elsevier Science B.V. All rights reserved.