Magnetic properties and exchange coupling of Nd-Ce-Fe-B nanocomposite films
Magnetic properties and exchange coupling of Nd-Ce-Fe-B nanocomposite films
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Nd-Ce-Fe-B纳米复合薄膜的磁性能及交换耦合
DOI:
10.7498/aps.66.157502
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发表时间:
2017-08-05
影响因子:
1
通讯作者:
Li Wei
中科院分区:
文献类型:
--
作者:
Sun Ya-Chao;Zhu Ming-Gang;Li Wei
In the early 1980 s, the soft and hard magnetic nano-two-phase permanent magnet materials were developed and exchange coupling model was put forward. Moreover, the theoretical maximum magnetic energy product could reach 120 MGOe (1 Oe = 7 9 : 5 7 7 5 A/m). However a great many of experimental research results are always disappointing for theoretical calculation, but previous studies have shown that there exists also a strong exchange coupling in hard magnetic phase, which can improve the magnetic property of magnet.In this paper, nanocomposite Ta(50 nm)/NdFeB(100 nm)/Ta(2 nm)/NdCeFeB(100 nm)/Ta(2 nm)/NdFeB(100 nm)/ Ta(40 nm) multilayer films with Ta underlayers and coverlayers are fabricated on Si substrates by direct current sputtering. A 50 nm Ta underlayer and a 40 nm coverlayer are sputtered at room temperature to align the easy axis of the RE2Fe14B grains to the direction perpendicular to the film plane and to prevent the magnetic film from oxidizing, respectively. The 2 nm Ta spacer layer serves as suppressing the diffusion of elements between different magnetic layers. The NdFeB and NdCeFeB magnetic film are deposited at 630 degrees C and 610 degrees C, respectively, and then they are followed by in situ rapid thermal annealing at 645-705 degrees C for 30 min. The microstructures and morphologies of the films are characterized by X-ray diffractometry with Cu K-alpha radiation, atomic force microscope, and magnetic force microscope. The magnetic properties of the films are measured with vibrating sample magnetometer.The influences of annealing temperature on magnetic property and crystal structure of the film are investigated. The results show that the magnetic property of the film improves gradually with the increase of annealing temperature, but deteriorates sharply when the temperature reaches above 695 degrees C. When the annealing temperature is 675 degrees C, the coercivity H-ci of the film reaches 10.1 kOe and the remanence 4(pi)M(r perpendicular to) is 5.91 kG (1 G = 10 3 /(4 pi) A/m), with a magnetic field applied to the direction perpendicular to the plane of the Nd-Ce-Fe-B thin film. The X-ray diffraction results show that the grains of the hard magnetic phase (2 : 1 4 : 1 phase) grow almost along the substrate normal (c-axis direction), of course, with a certain misorientation. Through the magnetization reversal process of the Nd-Ce-Fe-B thin film, it is found that the minimum value of M rev moves in the direction of decreasing M irr as the applied magnetic field increases, which is similar to the domain wall bowing model. This indicates that there is a strong local domain wall pinning in the film. Moreover, the remanence curve shows that the pinning type mechanism is indeed not dominant in the magnetization reversal process of the Nd-Ce-Fe-B thin film after annealing at 685 degrees C. In addition, Henkel plots are also investigated in the films at different annealing temperatures. It is believed that nonzero delta(m) is due to the interaction between particles in the magnet. It can be stated based on the measuring results that there exists a strong magnetic exchange coupling effect in the Nd-Ce-Fe-B thin film.