X-ray absorption spectroscopic and magnetic characterization of cobalt-doped zinc oxide nanocrystals prepared by the molten-salt method

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Abstract

The local atomic arrangement and electronic structure of the Co-doped Zn1−xCoxO nanocrystal have been quantitatively examined along with its magnetic properties. According to our analysis using powder X-ray diffraction, electron microscopy, and Zn K-edge X-ray absorption spectroscopy (XAS), phase-pure wurzite-structured Zn1−xCoxO nanocrystals have been successfully synthesized via the molten-salt method. The Co K-edge XAS analysis clearly demonstrates that all the Co2+ ions are substituted for the tetrahedral Zn sites of the Wurzite structure with a coordination number of 3.9 and a bond distance of 1.97 Å, ruling out the presence of magnetic impurity phase and Co-metal cluster. Magnetization measurements reveal that the present Zn1−xCoxO sample does not show any ferromagnetic transition down to 2 K. In this regard, we can conclude that Co-doped zinc oxide is not ferromagnetic but the previously reported ferromagnetism in this phase would be an extrinsic property.

Introduction

Over the last decade, diluted magnetic semiconductors (DMSs) have attracted special attention because of their unique ferromagnetism at room temperature, applicable for spintronics [1]. The discovery of ferromagnetism above room temperature in Co-doped TiO2 has triggered a worldwide pursuit of new DMS materials [2]. The theoretical calculations by Sato and Katayama-Yoshida [3] showed that ZnO doped with several 3d transition metal ions such as V, Cr, Fe, Co and Ni may exhibit ferromagnetic ordering. In fact, many researchers have reported experimental evidence on the ferromagnetism of Co-doped ZnO materials near or above room temperature [4], [5], [6]. However, there are considerable numbers of contradictory reports claiming the absence of ferromagnetism in this system [7], [8]. Also, it was supposed that the ferromagnetism of Zn1−xCoxO would stem from extrinsic factors like the existence of magnetic impurity phase. This suggestion was supported by the first principle calculation results showing that Co-doped ZnO prefers to be in a spin-glass state due to antiferromagnetic super-exchange interactions [9]. The above discussions demonstrate that the magnetic properties of Co-doped ZnO are by no means established. To obtain an insight into the relationship between magnetic properties and preparation condition, we made careful survey on the existing literatures about the DMS, which reveal that most Zn1−xCoxO samples showing ferromagnetism were prepared by a high-temperature heat treatment. The sintering at elevated temperature might produce Co-based magnetic impurity phases. Furthermore, magnetization values reported by many workers are too small to be attributable to the bulk ferromagnetism of Zn1−xCoxO [10], supporting the presence of magnetic impurities. In this regard, it is of crucial importance not only to synthesize single-phase Zn1−xCoxO without the formation of the Co-containing impurity phase but also to quantitatively characterize the local crystal structures of doped cobalt ions for clarifying uncertainty about the ferromagnetism of Co-doped Zn1−xCoxO.

In this study, we have quantitatively studied the local structure and oxidation state of zinc and cobalt ions in phase-pure Co-doped Zn1−xCoxO samples prepared by a molten-salt method. We chose the molten-salt flux method because it is known to be capable of producing highly crystalline phase-pure materials in large scales, and has been employed in the syntheses of various oxide materials, where features are desirable for the purpose of the present study [11], [12]. With a reference to the experimental data of reference CoO, Co K-edge extended X-ray absorption fine structure (EXAFS) analysis allows us to exactly determine the coordination number and local atomic arrangement of cobalt ions doped in zinc-oxide lattice.

Section snippets

Experimental

The Co-doped Zn1−xCoxO sample was synthesized by the molten-salt method. The precursor was prepared by grinding a mixture of Zn(Ac)2·2H2O, Co(Ac)2·4H2O, 2.5 mL nonylphenol ethoxylate surfactant, oxalic acid and aged at 60 °C for 6 h. The precursor was washed with water and acetone for several times, separated by centrifugation, and dried at 80 °C. Typically 1 g of the precursor was mixed with 4 g NaCl. The mixture was heated at 910 °C for 2 h, and then cooled to room temperature at a rate of 5 °C/min.

Powder XRD and FE-SEM analyses

Fig. 1a represents the powder XRD pattern of the Co-doped Zn0.95Co0.05O sample. All of the observed diffraction peaks could be well indexed on the basis of the Wurzite structure with the hexagonal symmetry. No impurity phases could be detected. The particle size and crystallite morphology of the Zn0.95Co0.05O compound were examined using FE-SEM, as illustrated in Fig. 1b. The present compound shows a pseudo-spherical morphology with the particle size of 200–300 nm.

Zn K-edge XANES analysis

We have investigated the

Conclusions

We have investigated the local crystal and electronic structures of zinc and cobalt ions in Co-doped zinc oxide Zn1−xCoxO nanocrystal as well as its magnetic properties. Zn K- and Co K-edge XAS analyses clearly demonstrate that divalent zinc and divalent cobalt ions are commonly stabilized in the tetrahedral sites of the Wurzite structure without the formation of magnetic impurity phase. From the magnetization measurements, it was found that the Co-doped zinc oxide does not show any

Acknowledgments

This work was supported by the Korea Research Foundation Grant funded by the Korean Government (MOEHRD)” (KRF-2005-005-J11903), CNNC (at SKKU) and by the Ministry of Environment (Grant No.: 022-061-023). The experiments at PAL were supported in part by MOST and POSTECH.

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