Elsevier

Ceramics International

Volume 40, Issue 6, July 2014, Pages 7753-7759
Ceramics International

Synthesis and characterization of Mn-doped ZnO nanorods grown in an ordered periodic honeycomb pattern using nanosphere lithography

https://doi.org/10.1016/j.ceramint.2013.12.117Get rights and content

Abstract

We report a study of the structural, optical and magnetic properties of undoped and Mn-doped ZnO nanorods grown by chemical bath deposition in a periodic honeycomb lattice formation. Mn-doping is accomplished by a diffusion process at a constant time of 8 h for different temperatures of 500 °C, 600 °C and 700 °C. Undoped and Mn-doped ZnO nanorods had a hexagonal wurtzite structure with a (0 0 2) preferred orientation. From SEM results, it was seen that Mn-doped ZnO nanorods grew vertically in the honeycomb lattice with lengths of 0.8 μm. XPS results showed that Mn3+ ions was successfully incorporated in the ZnO matrix by substituting for Zn2+ ions and that Mn-doping increased the number of oxygen vacancies in ZnO compared to undoped ZnO. This result was also supported by photoluminescence data at 10 K. Magnetic data showed that all the samples exhibited ferromagnetic character. Although the origin of undoped ZnO is related to oxygen vacancy-induced d0 ferromagnetism, bound magnetic polarons are responsible from the ferromagnetism of Mn-doped ZnO samples which have Tc values above the room temperature.

Introduction

In recent years, diluted magnetic semiconductors (DMS) have attracted significant interest due to their potential applications in spintronic devices. Among II–VI group semiconductors, especially, ZnO has gained lots of interest since it has a wide band gap of 3.37 eV with an excitonic binding energy of 60 meV at room temperature that make it an important material for potential optoelectronic applications [1]. ZnO is also a promising material in the investigation of DMS systems that can be achieved by doping with 3-d group elements like Mn, Co, Fe etc. and by these means the optical and magnetic properties of ZnO materials can be tuned. In particular, Mn-doped ZnO nanostructures have attracted significant interest as Mn has the highest magnetic moment and the first half of the d band is fully occupied [2]. The literature contains some reports of experimental studies on ZnO:Mn grown with diverse morphologies such as thin films, nanocrystals and nanowires and exhibiting room temperature ferromagnetism. For instance, Yang et al. produced Mn-doped ZnO thin films by the sol–gel technique on both glass and Si substrates and they found that even though undoped ZnO exhibited diamagnetic behavior, all the ZnO:Mn samples had a ferromagnetic character at room temperature. The origin of ferromagnetism was explained by the substitution of Mn2+ ions on Zn2+ sites [3]. Sain et al. synthesized ZnO:Mn nanocrystalline samples by mechanical alloying using a mixture of ZnO and MnO powders for different doping concentrations and room temperature ferromagnetism for ZnO:Mn samples was obtained. The origin of ferromagnetism was attributed to RKKY exchange interactions [4]. Furthermore, Philipose et al. grew ZnO:Mn nanowires by the vapor phase transport technique on Au-catalyzed Si substrates with Mn concentrations of 1 at%, 2 at% and 4 at%. They observed room temperature ferromagnetic character for 1 at% Mn-doping and the ferromagnetism was attributed to the interactions between Mn ions and native defects [5].

ZnO material doped with transition-metal (TM) ions has been grown in various morphologies such as nanowires, nanorods and nanotubes [6], [7], [8]. Some methods to deposit TM-doped 1-D ZnO nanostructures include RF magnetron sputtering [9], vapor phase transport [10], pulsed laser deposition [11], spray pyrolysis [12] and chemical bath deposition (CBD) [13]. Among these methods, CBD is an attractive technique and offers advantages such as simple, low cost equipment and a low growth temperature [14]. To the best of our knowledge, this is the first study investigating the structural, optical and magnetic properties of Mn-doped ZnO nanorods grown into a periodic honeycomb pattern. Additionally, the study focuses on clarifying the origin of room temperature ferromagnetism observed in both undoped and Mn-doped ZnO nanorods grown this honeycomb lattice using both photoluminescence and X-ray photoelectron spectroscopy results.

Section snippets

Experimental details

The experimental details concerning the growth of a ZnO buffer layer on Si substrates using both a seed layer followed by chemical bath deposition (CBD) can be found in [10]. To ensure spatially ordered nanostructure growth, ZnO buffer layer coated Si substrates were patterned using a modified nanosphere lithography (NSL) technique [15] whereby a close packed monolayer of polystyrene nanospheres (diameter 1 µm) are deposited on the sample. This nanosphere layer is then used as a template for a

Results and discussion

Fig. 1(a)–(d) shows the XRD patterns of undoped and Mn-doped ZnO nanorods annealed at 500 °C, 600 °C and 700 °C for 8 h in vacuum, respectively. In all cases a dominant peak at 34.4° is seen, corresponding to the ZnO (0 0 2) reflection (JCPDS card no:36-1451), confirming the deposit as ZnO material with the normal hexagonal wurtzite structure. As seen from the figure, the strong (0 0 2) preferred orientation perpendicular to the substrate was observed for all the samples, indicating a highly textured

Conclusions

In conclusion, the results of the study can be summarized as follows: (i) XRD data showed that all the samples had a (0 0 2) preferential orientation perpendicular to the substrate; (ii) SEM results indicated that undoped and Mn-doped ZnO nanorods were successfully grown in the periodic honeycomb pattern; (iii) the valence state of Mn ions in the ZnO was determined to be +3, indicating that Mn substitutes for Zn in the ZnO lattice, consistent with XRD data also; (iv) it was found from optical

Acknowledgement

The first and corresponding author (SY) of the study would like to thank the Turkish Higher Education Council for its financial support to visit Dublin City University for an extended research stay. All the magnetic measurements reported in the study were carried out by Assoc. Prof. Dr. A. Ceylan and Prof. Dr. Ş. Özcan (Hacettepe University). All the authors are also grateful to Dr. M. Çopuroğlu and Prof. Dr. Ş. Süzer (Bilkent University) for XPS measurements.

References (33)

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