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Abstract

Contents

Introduction

As an essential member of functional materials, permanent magnetic materials have been widely used in many major industries [1-3]. Until now, permanent magnet materials have gone through five stages, carbon steel, Al-Ni-Co alloy, permanent magnet ferrites, Sm-Co alloy series and Nd-Fe-B series. 1-1 [7] shows the development and magnetic properties of these five kinds of permanent magnetic materials.

Among these materials, the production of carbon steel was almost stopped, Al-Ni-Co alloy was widely used in precision instruments due to its outstanding temperature stability, and Nd-Fe-B magnets were mainly used in some advanced equipment, considering both its amazing magnetic properties and high price; compared to Nd-Fe-B magnets, Sm-Co magnets have not so good properties, but much higher Currie temperature (Tc). Ferrites, as part of permanent magnetic material, have high performance and cost efficiency due to their relatively cheap raw materials, easier manufacturing process and good magnetic properties [1-4]. To enhance the magnetic properties of SrM, many methods have been tried, one effective method is to use rare earth ions to replace Sr2+ ions because the radius of Sr2+ ions is 0.127 nm close to the radius of O2- ions of 0.132 nm, so that Ca2+, Na+ and K+ ions and rare earth element ions can partially or completely replace Sr2+ ions.

In this study, Sr-La M-type ferrites were synthesized by a conventional solid-state method with an iron deficiency factor y to enhance ion diffusion and improve the associated magnetic properties. We report on the effect of iron deficiency on the microstructure and magnetic properties of Sr-La hexaferrites.

Background

  • Crystal structure of M-type hexaferrites
  • Magnetic properties of M-type hexaferrites
  • Cation substitution of M-type hexaferrites

Saturation magnetization (Ms) is a condition where an increasing applied external magnetic field H cannot increase the magnetization of the material any further, so that the total magnetic flux density B more or less levels out. The molecular magnetic moment from a molecule of SrFe12O19 occupying half of the unit cell consists of SRS*R* blocks, which contain two SrFe12O19. The coercivity (Hc), also called magnetic coercivity, coercive field or coercive force, is a measure of a magnetic material's resistance to magnetization change, corresponding to the field intensity needed to demagnetize the fully magnetized material.

So, it is important to increase Ms without obvious decrease in Hc, which is closely related to the magnetocrystalline anisotropy (MCA) and grain size. These directions are usually related to the principal axes of its crystal lattice, for SrM, the c-axis [0001]. It is not enough to only control factors such as ball milling time, ball to raw material ratio, calcination and sintering temperature, heat preservation time and press quality, reports indicated that by substituting certain ions in ferrites, the magnetic properties can be improved to the next level, and some of them even reached the theoretical value, in this case ion substitution is a very effective method for magnetic property improvement of hexaferrites.

The reason for the improvement is that the rare earth ions have a close-packed double hexagonal crystal structure, which leads to the strong magnetic anisotropy. Co2+-Ti4+ co-substituted Fe3+ induced decrease in coercivity without changing saturation magnetization.

Experimental

  • Synthesis of Sr-La hexaferrites
  • Characterization

Since studies of ferrites with La ratio x no more than 0.4 have been widely reported, D.seifer et al. also reported at 1300 °C La has the maximum solubility of 0.5[13] so the La ratio was fixed at x= 0.5 to check the effect of iron deficiency on phase ratio of Sr0.5La0.5Fe12-yO19 -δ hexaferrites. 4-3 showed, no obvious characteristic diffraction peaks of other phases could be found in the XRD patterns. Lattice parameters a and c were calculated from the values ​​of dhkl according to the following equation.

On the other hand, for these single-phase samples, increasing iron deficiency implies a higher ratio of Fe2+ ions to all Fe ions, and Fe2+ ions with a larger ion radius can increase the lattice parameter c, due to to these factors the lattice parameter c was first decreased and then increased, samples as shown in Fig. Lattice parameters and unit cell volumes of Sr0.5La0.5Fe12-yO19-δ samples versus Fe content. At 1300°C the sample with Fe content of 11.75 has the lowest lattice parameter c and unit cell volume values.

M MS B H (4-4) Therefore, in a strongly applied magnetic field, the M-H curves are fitted with equation (4-4), allowing the values ​​of the saturation magnetization Ms to be calculated. The positive and negative values ​​of the Hc and Mr can be read accordingly from the hysteresis loops, the average value between them being the Hc and Mr values. The second factor from iron deficiency to saturation magnetization is the increasing iron deficiency, which decreases the number of iron ions with spin-up orientation and weakens the superexchange interaction. The iron deficiency also leads to a higher La3+ to Fe3+ ratio and weakens the so-called tilting spin structure. , leading to a decrease in saturation magnetization.

The possible reason for the low Hc could be that the internal coercivity decreased when the temperature rose, that magnetic alignment became more difficult and the particles grew larger. The effect of iron deficiency on the microstructure and magnetic properties of Sr0.5La0.5Fe12-yO19-δ was investigated. Thus, iron deficiency can be a beneficial factor for the synthesis of single-phase Sr-La M-type hexagonal ferrites as well as Sr-La-Co M-type ferrites.

Second, for single-phase Sr0.5La0.5Fe12-yO19-δ ferrites sintered at 1300 °C for 2 h in air, the lattice parameters a, c and unit cell volume all decreased initially but increased later with the growth of y. SEM investigations revealed that the average grain size of the sample with the same sintering condition was about 2 μm and shows a decreasing trend with iron deficiency when sintered at 1300 °C for 2 h. Also, as y increases, the saturation magnetization Ms is about 70 emu/g, but Hc decreased compared to the previous report, which may be a defect effect of high temperature.

Iron deficiency can lead to the production of iron and oxygen vacancies, which can improve the diffusion between various ions. The magnetic properties of Sr-La increased slightly with iron deficiency, the optimal Ms of 72.8 emu/g was obtainable with a coercivity of 3300 Oe for this Sr0.5La0.5Fe12-yO19-δ sample sintered at 1325˚C for 2 hours in air.

Results and Discussion

  • Crystal structure of Sr 0.5 La 0.5 Fe 12-y O 19-δ
  • Microstructure and morphology of Sr 0.5 La 0.5 Fe 12-y O 19
  • Magnetic properties of Sr 0.5 La 0.5 Fe 12-y O 19-δ

Conclusion

In this study, Sr1-xLaxFe12O19 and Sr0.5La0.5Fe12-yO19-δ were synthesized by conventional ceramic reaction. Sr-La M-type single-phase hexaferrites with a Sr/Fe ion ratio of 0.5/0.5 have never been reported. The properties of ferrites have been synthesized, implying that it should be a promising alternative to the current M-type hexaferrites for permanent magnet applications.

우리는 헥사페라이트의 자기적 특성을 연구했습니다. 제조된 시료의 결정구조는 XRD를 통해 확인하였고, 미세구조는 FE-SEM을 통해 확인하였다. VSM을 통해 자기적 특성을 확인하였습니다.

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