Abstract

Zn0.98–yEr0.02AlyO (0 ≤ y ≤ 0.04) thin films have been prepared by inductively coupled plasma enhanced physical vapor deposition method. It is found that Er3+ substitutes Zn2+ in ZnO lattice without forming any magnetic secondary phase. Al-doping has dual effects on the electron transport and magnetic properties of Er-doped ZnO films, wherein AlZn and Ali play different roles. When 0 ≤ y ≤ 0.02, the dominant AlZn increases and induces both carrier concentration and saturation magnetization (Ms) increasing. When 0.02 < y ≤ 0.04, Ali becomes main defect and enhances the probability of electron scattering, thus reduces the Ms.

Highlights

  • There is tremendous flurry of research interest in diluted magnetic semiconductors (DMSs) for its potential application in spintronics.[1,2,3,4] It is because charge and spin of carriers can be simultaneously controlled in DMSs

  • For the Zn0.98–yEr0.02AlyO (0 ≤ y ≤ 0.04) thin films in this study, an obvious increase of c-axis length is observed in Fig. 1(b) after y > 0.02, which indicates that the ratio of Ali to AlZn may dramatically raise when the Al concentration is larger than 2 at.%

  • Room-temperature ferromagnetism has been obtained in Zn0.98–yEr0.02AlyO (0 ≤ y ≤ 0.04) thin films prepared by inductively coupled plasma enhanced physical vapor deposition (ICP-PVD) method

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Summary

INTRODUCTION

There is tremendous flurry of research interest in diluted magnetic semiconductors (DMSs) for its potential application in spintronics.[1,2,3,4] It is because charge and spin of carriers can be simultaneously controlled in DMSs. Et al.[9,10] reported that Er-doped ZnO thin films exhibited room-temperature ferromagnetism and the ferromagnetism originated from Er substitution for Zn in ZnO lattice, while the effect of carrier concentration is not mentioned. Since Al-doping is able to increase carrier concentration in transition metals-doped ZnO, it is promising for modifying the magnetism. Some researchers have reported that Aldoping can increase the saturation magnetization (Ms) of Co-doped ZnO14,15 and Fe-doped ZnO16 due to the increase of carrier concentration. The role of Al-doping in the magnetism of Er-doped ZnO thin films still remains obscure. A series of experiments were designed to illustrate the ferromagnetism origin in the Er-doped ZnO system and to clarify the function of Al in Zn0.98–yEr0.02AlyO thin films

EXPERIMENT
RESULTS AND DISCUSSION
CONCLUSIONS
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