Structural and magnetic properties of annealed FePt/Ag/FePt thin films

被引:23
|
作者
Pavlova, O. P. [1 ]
Verbitska, T. I. [1 ]
Vladymyrskyi, I. A. [1 ]
Sidorenko, S. I. [1 ,2 ]
Katona, G. L. [2 ]
Beke, D. L. [2 ]
Beddies, G. [3 ]
Albrecht, M. [3 ]
Makogon, I. M. [1 ]
机构
[1] Natl Tech Univ Ukraine, Kyiv Polytech Inst, UA-03056 Kiev, Ukraine
[2] Univ Debrecen, Dept Solid State Phys, H-4010 Debrecen, Hungary
[3] Tech Univ Chemnitz, Inst Phys, D-09126 Chemnitz, Germany
基金
匈牙利科学研究基金会;
关键词
L1(0) FePt; Chemical ordering; Secondary neutral mass spectrometry; Magnetic coercivity; FEPT;
D O I
10.1016/j.apsusc.2012.11.102
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
Layer stacks of FePt(15 nm)/Ag(x)/FePt(15 nm) with various Ag interlayer thicknesses (x = 0, 3, and 30 nm) were deposited at room temperature onto SiO2(100 nm)/Si(0 0 1) substrates. These films were post-annealed in a temperature range of 100 degrees C-900 degrees C for 30 s under high vacuum condition. The influence of the Ag interlayer on the L1(0)(FePt)(FCT) phase formation and its related structural and magnetic properties were investigated. The onset of chemical ordering of FePt single layers is observed at annealing temperatures between 600 degrees C and 700 degrees C. Increasing the Ag interlayer thickness to 30 nm reduces the ordering temperature of the L1(0)(FePt)(FCT) phase formation by about similar to 100 degrees C. Higher annealing temperatures lead to a further increase in volume fraction of the ordered L1(0)(FePt)(FCT) phase but also to the diffusion of Ag towards the free surface as probed by secondary neutral mass spectrometry. In addition, due to the limited solvability of Ag into the FePt phase, Ag is expected to be located at the grain boundaries. The increasing volume fraction of the L1(0)(FePt)(FCT) phase is also reflected in the increasing coercivity of the films which reaches values of up to similar to 19 kOe after annealing at 900 degrees C. Furthermore, in this case similar M-H hysteresis loop were recorded when the field is applied in the film plane and perpendicular to it. This isotropic behavior is in agreement with the coexistence of L1(0) ordered grains which are randomly oriented. (c) 2012 Elsevier B.V. All rights reserved.
引用
收藏
页码:100 / 104
页数:5
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