- Nano Express
- Open Access
Synthesis, Magnetic Anisotropy and Optical Properties of Preferred Oriented Zinc Ferrite Nanowire Arrays
© The Author(s) 2010
- Received: 10 April 2010
- Accepted: 6 May 2010
- Published: 22 May 2010
Preferred oriented ZnFe2O4 nanowire arrays with an average diameter of 16 nm were fabricated by post-annealing of ZnFe2 nanowires within anodic aluminum oxide templates in atmosphere. Selected area electron diffraction and X-ray diffraction exhibit that the nanowires are in cubic spinel-type structure with a  preferred crystallite orientation. Magnetic measurement indicates that the as-prepared ZnFe2O4 nanowire arrays reveal uniaxial magnetic anisotropy, and the easy magnetization direction is parallel to the axis of nanowire. The optical properties show the ZnFe2O4 nanowire arrays give out 370–520 nm blue-violet light, and their UV absorption edge is around 700 nm. The estimated values of direct and indirect band gaps for the nanowires are 2.23 and 1.73 eV, respectively.
- Nanowire arrays
- Preferred oriented
- Magnetic anisotropy
- Optical properties
As an important member of ferrite family, nanometer-sized spinel ZnFe2O4 has received growing interest from the fundamental and experimental point of view because of its potential application in gas sensors with high sensitivity and low-energy consumption [1–4]. Besides, the nanometer-sized ZnFe2O4 is considered as a promising semiconductor photocatalyst for various photochemical processes, such as photoelectric conversion and photochemical hydrogen production from water, owing to its ability to absorb visible light, high efficiency, low cost, and excellently photochemical stability [5–7]. Meanwhile, the nanometer-sized ZnFe2O4 shows unusual magnetic properties compared to the bulk form , such as high Curie temperature and large magnetization at room temperature (RT) have been observed in ZnFe2O4 nanoparticles and films [9–12]. The issue has been extensively researched and ascribed to the dominant role of oxygen vacancies , surface effects , as well as cation random distribution of magnetic Fe3+ ions and diamagnetic Zn2+ ions among the interstitial octahedral (B) and tetrahedral (A) sites .
One-dimensional nanostructures can provide versatile building blocks for fabricating functional nanoscale electronic, optoelectronic, biomedical devices, magnetic and optical properties based on the bottom-up paradigm [16–20]. Recently, arrays of Ru, Pt, and PtRu nanowires and nanotubes were prepared by electrodeposition through the porous structure of an anodic aluminum oxide (AAO) membrane . Iron-based 1D nanostructures have been successfully prepared using an electrospinning technique and varying the pyrolysis atmospheres . Besides,1D magnetic MFe2O4 (M = Co, Ni and Mn) nanomaterials also have been fabricated owing to their unique application in mesoscopic physics and nanoscale devices excellent properties [23–25]. For zinc ferrite, Liu et al. fabricated ZnFe2O4 nanowires exhibiting unusual magnetic behavior by the thermal decomposition of the precursors inside silica host SBA-15 template . By using a facile sol–gel AAO template method, Zhang and Liu et al. got highly ordered ZnFe2O4 nanotube arrays, which displayed low-energy consumption and high sensitivity to organics as gas sensor materials and exhibited unusual photovoltaic behavior [7, 27]. However, all these 1D ZnFe2O4 nanostructures have no orientation, where Kim et al. demonstrated that ordered ZnO microrod arrays with the preferred orientation of  direction showing a strong free-exciton emission at 3.23 eV and a weak deep level emission at 2.2 eV reveals the high optical quality than that of the ZnO nanowire arrays with no orientation [28, 29].
Recently, Zhang and Zhu et al. demonstrated that the properties of 1D nanostructures depend strongly not only on the ordered arrangement but also on the crystal orientation as well [30, 31]. In our previous, the ordered CoFe2O4 nanowire arrays with preferred crystal orientation were prepared by using the template synthesis in conjunction with electrochemical deposition . Here, ordered ZnFe2O4 nanowire arrays with preferred crystal orientation of  direction were prepared by spatial confinement oxidation of preferred  crystal orientation ZnFe2 alloy nanowires in AAO templates. The magnetic and optical properties of ZnFe2O4 nanowire arrays were studied.
AAO was used as the template to synthesize ZnFe2O4 nanowire arrays. The AAO templates were prepared through two anodizing steps as our report previously . Briefly, high purity (99.999%) aluminum foil was polished in the mixed solution of ethanol and choric acid (HClO4) in the constant current of 1.5 A for 5 min. The two-step anodization process was carried out in constant voltage mode to improve the arrangement of the ordered nanopore arrays. In the first step of the anodization, aluminum foil was anodized in 0.3 M H2SO4 aqueous solution under the constant voltage of 13 V at 0°C for 0.5 h resulting in the textured surface, and then the formed anodic alumina layer was removed in the mixed solution of 0.4 M phosphoric acid and 0.2 M chromic acid at 60°C. Subsequently, the foil was re-anodized for 4 h using the same parameters in the first step. The electrolyte contained FeSO4·7H2O (22 g/l), ZnSO4·7H2O (10 g/l), H3BO3 (10 g/l) with the pH value of 3.2. The alternating current electrodeposition was conducted at 200 Hz and 13 V for the duration of 5 min. The compositions in the ZnFe alloy nanowires were analyzed by energy dispersive X-ray spectroscopy (EDS) and inductively coupled plasma-atomic emission spectrometer (IRIS, ER/S). The results indicate the atom ratio of Fe:Zn is about 2. Because of the confinement of the nanopore size, after heat treating the well orientation ZnFe2 alloy nanowire arrays in tube furnace at 460°C for 21 h in atmosphere, the arrays of ZnFe2O4 nanowires inside the AAO templates with preferred crystallite orientation were obtained.
The morphologies of the nanowires were obtained by using the scanning electron microscope (SEM, Hitachi S-4800) and transmission electron microscopy (TEM, JEM-2010), where the nanowires were separated from the AAO templates by dissolving the aluminium oxide templates in the mixed solution of 0.2 M H2CrO4 and 0.4 M H3PO4. The selected area electron diffraction (SAED) and X-ray diffraction (XRD, X’ Pert PRO PHILIPS with Cu Kα radiation) were employed to study the structure of the nanowires. The measurements of magnetic properties were made using Quantum Design MPMS magnetometer based on superconducting quantum interference device (SQUID) and vibrating sample magnetometer (VSM, Lakeshore 7304). Micro photoluminescence (PL) measurement was carried out at room temperature (RT) using a He-Cd laser with the wavelength of 325 nm and output power of 15 W as the excitation source. Light absorption property was measured using a UV–vis spectrophotometer (JASCO, UV-550).
The schematic of the possible formation process of preferred oriented ZnFe2O4 nanowire arrays is shown in Fig. 2c. The process could be described as: ZnFe2 + 2O2 → ZnFe2O4. The XRD result shows that the ZnFe2 alloy nanowires have the preferred  crystal orientation along the axis of nanowires, which combined with the minor holes of AAO templates playing an important role to make the growth of ZnFe2O4 nanowire arrays largely guide along the nanowire axis direction when heat treated. To sum up, there are two main conditions that make the nanowire arrays prefer crystal orientation: the one is the well orientation of original metal crystal, and the other is the spatial confinement of the minor hole.
As we known, bulk Zn-ferrite belongs to the normal spinel structure with paramagnetic properties at RT and long range antiferromagnetic order below 10 K . However, nanocrystalline zinc ferrite is of great interest due to its unique magnetic properties that differ substantially from its bulk counterpart . The occupancy of Fe3+ ions on both A- and B-sites leads to strong negative superexchange interaction between Fe3+ ions with large magnetization values. In our experiment, when ZnFe2 alloy nanowires were post-oxidation annealed, defects and the disorder of cation redistribution on A- and B- sites may occur, which can induce the magnetization for ZnFe2O4 nanowire arrays in our case.
In summary, arrays of ZnFe2O4 nanowires with diameters of about 16 nm were successfully fabricated by electrodeposition of Zn2+ and Fe2+ into AAO templates and post-oxidation annealing in atmosphere. The results of XRD and HRTEM exhibit that the nanowires have the bcc structure with  as the texture direction along the nanowire axis. The preferred orientation and shape anisotropy of the nanowire arrays makes the ZnFe2O4 nanowire arrays to exhibit the uniaxial magnetic anisotropy with the easy magnetization direction along the nanowire axes. The optical properties show ZnFe2O4 nanowire arrays give out blue-violet light, and the optical band gap E g is estimated from absorption coefficient. Further investigation into magnetic and optical properties of the ZnFe2O4 nanomaterials is in progress.
This work is supported by National Science Fund for Distinguished Young Scholars (Grant No. 50925103), The Keygrant Project of Chinese Ministry of Education (Grant No. 309027) and The Fundamental Research Funds for the Central Universities (Grant No. Lzujbky-2009-162).
This article is distributed under the terms of the Creative Commons Attribution Noncommercial License which permits any noncommercial use, distribution, and reproduction in any medium, provided the original author(s) and source are credited.
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