• Aucun résultat trouvé

STRUCTURAL AND MAGNETIC PROPERTIES IN MnBiAlSi AND MnBiSbSi FILMS

N/A
N/A
Protected

Academic year: 2021

Partager "STRUCTURAL AND MAGNETIC PROPERTIES IN MnBiAlSi AND MnBiSbSi FILMS"

Copied!
3
0
0

Texte intégral

(1)

HAL Id: jpa-00229035

https://hal.archives-ouvertes.fr/jpa-00229035

Submitted on 1 Jan 1988

HAL is a multi-disciplinary open access

archive for the deposit and dissemination of

sci-entific research documents, whether they are

pub-lished or not. The documents may come from

teaching and research institutions in France or

abroad, or from public or private research centers.

L’archive ouverte pluridisciplinaire HAL, est

destinée au dépôt et à la diffusion de documents

scientifiques de niveau recherche, publiés ou non,

émanant des établissements d’enseignement et de

recherche français ou étrangers, des laboratoires

publics ou privés.

STRUCTURAL AND MAGNETIC PROPERTIES IN

MnBiAlSi AND MnBiSbSi FILMS

Y. Wang, J. Shen, Q. Tang

To cite this version:

(2)

JOURNAL DE PHYSIQUE

Colloque C8, Suppl6ment a u no 12, Tome 49, dBcembre 1988

STRUCTURAL AND MAGNETIC PROPERTIES IN MnBiAlSi AND MnBiSbSi FILMS

Y. J. Wang, J. X. Shen and Q. Tang

Institute of Physics, Chinese Academy of Sciences, Beijing 100080, China

Abstract.

-

The thermal structural stability and the crystallite size in MnBi could be much improved after it is doped by Al, Si or Sb, Si. However, the large Kerr rotation angle Bk in MnBi is maintained in the new constitution, especialy in MnBiAlSi films. Therefore, it is a promising material for the magneto-optical recording.

Introduction

In recent years, many efforts have been devoted to develop new media for magnetic optical disc applica- tions, but it seems that materials with good qualities such as large read-out signal, thermal stability a d low noise are difficult t o find.

In the present paper, results on a new kind of magneto-optical medium, MnBi-base films, will be pre- sented.

Experimental

By vacuum evaporation (I), MnBiAlSi, MnBiSbSi films were prepared. The base pressure of vacuum sys- tem is about 3 x Torr. In order to obtain ho- mogeneous MnBi-base alloy films, a heat treatment in vacuum is required.

The magnetic properties, saturation magnetization

M,, perpendicular anisotropy constant K,, coercive

force Hc and Kerr rotation angle Ok were determined

by vibrating sample magnetometer, Torque measure- ment and magneto-optical spectra at 633 nm respecti- vely.

Results

The X-ray diffraction of MnBiAlSi film with an ap- propriate constitution shows that it has a perfect hexa- g o d structure with NiAs type, that is, the c axis is perpendicular to the basal plane (see Fig. 1).

Figure 2 gives the Auger electron spectroscopy pro- file for this film. It is clear that a considerable amounts of Al, Si and 0 enter in the MnBi hexagonal structure. According t o the X-ray diffraction, they are not found in ordered phases.

e k , R (reflectivity),

K,,

Ma and H, for the opti-

mal MnBiAlSi composition were determined to be Ok=

1.2 deg., R = 40 %, ~,=2.2x10' erg/cc, Hc=1800 Oe and M,=250 emu/cc. The signal to be picked up in magneto-optical disc is proportional t o O k f i . It is no- ticed that this value in the MnBiAlSi film could be increased by a factor of 3 as compared with the amor- phous R E T M films.

z e (d.,l.)

Fig. 1. - X-ray diffraction for MnBiAlSi film.

SPUTTER T I M E ( r n i n . )

Fig. 2. - AES profile for MnBiAlSi film.

.

""

8 0

As a magneto-optical recordidng medium, the ther- mal stability and the crystallite size in MnBi-base sys- tem are of much concern. Figure 3 gives the quenching experiments for 6k,

Ms

and Hc. It could be seen that the thermal structural stability for MnBiAlSi film is

-

A E S P R O F I L E

(3)

C8 - 1726 JOURNAL DE PHYSIQUE

-

MnBiAISI

---

MnBi

I '

Ms

*0° BEPORE QUENCH

I

Fig. 3.

-

Bk, Ms and Hc as the function of the quenching T Fig. 5.

-

X-ray diffraction for Mn0.s (Bi0.26Sbo.7S)0.6 film for both MnBi and MnBiAlSi film. All measurements were (because Si atoms exist as the interstitial ones, hence Si

made at room T. content is not inclusive in this chemical formula).

much better than that for MnBi. A transition electron microscope picture for determination of the crystallite size d in MnBiAlSi film is shown in figure 4. The ave- rage crystallite size d could be estimated to be less than 400

k

from this picture.

As compared with MnBiAISi film, 6k in MnBiSbSi film is smaller (6k=0.5 deg., R = 20 %) although its thermal structural stability is similar t o MnBiAlSi film.

In the X-ray diffraction at the optimal composition M n 0 . a ( B i ~ . ~ ~ S b o . 7 ~ ) ~ . ~ , we have found a set of X-ray peaks (see Fig. 5), 26 = 27.35, 48.8 and 62.5 deg.

These peaks do not exist in the NiAs type, it may be a CdI2 type hexagonal structure with c = 6.5

A

[2].

Discussion

Analysing the hexagonal structure with NiAs type, we were able to find six interstitial sites in the unit crystal cell. Therefore, Mn atoms can jump into the interstitial sites when MnBi is annealed above

T,

point and then quenched. As a result, M,, Bk in MnBi de- crease due t o the formation of a quenched high tem- perature phase 131.

In the MnBiAlSi film, a lot of foreign atoms fills up the interstitial sites, so that the phase transition could be affected. We speculate that the foreign atoms enter the grain boundaries as well, therefore, the crystallite size decreases.

Acknowledgment

This work is supported by the Joint Optical Disc Laboratory and the Magnetism Laboratory of the Chi- nese Academy of Sciences.

[I] Chen, D., J. Appl. Phys. 42 (1971) 3625. Fig. 4.

-

TEM observation for MnBiAlSi film deposited on

a Cu-grid slice after annealing at an appropriate temper* [2] Wang, Y. J., Shen, J. X., Tang, Q., to be publi- ture, its electron diffraction image as shown in this figure shed in J. Magn. Magn. Muter.

Références

Documents relatifs

We can explain this by the following argument: below the transition temperature, there exists a single large cluster of lattice spins with some isolated ”defects” (i. clusters

The specimens with a single layer type of TbFeCo films and/or a double layer type of Al/TbFeCo films on the substrates have been prepared in this study.. The com- position

- Short-period compositionally modulated Cu-Ni multilayers were studied by transmission electron microscopy and torque magnetometry.. A high density of embeded twins and

Static magnetic proper- ties were determined by a vibrating sample magne- tometer (VSM) while X-band ferromagnetic resonance (FMR) spectra were taken with the

At the higher doping ratios ( 2 3-10-4) the F e m i level EF lies in the band tail above the dangling bond levels, so that the recombination rate is determined by a transition

~?Fe hyperfine field decrease with decreasing thickness which indicates the existence of two iron sites. An in-plane uniaxial anisotropy is found for the 65 nm thick film. Finally

Abstract.- Several amorphous Ce-Fe and Pr-Fe alloys were prepared by means of vapour-deposition and their magnetic properties were studied.. The Cel-,Fe, alloys are

In order to investigate this possibility, we have carried out magnetic and transport measurements on a Pr 0.7 Sr 0.3 MnO 3 thin film, while varying the direction of the applied