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Room Temperature Doped Ferromagnetic Oxides:<br />
- A current Scenario Towards Magnetic p-n Junctions<br />
K.V.Rao<br />
Dept of Materials Science-Tmfy, Royal Institute of Technology,<br />
Stockholm, Sweden<br />
A goal of spintronics is to develop a semiconductor that can manipulate the magnetism of an electron. Adding the<br />
spin degree of freedom to electronics will provide significant versatility and functionality to future electronic<br />
products. Although many possible electronic components, like for example the magnetic switch (Ohno et al) have<br />
been demonstrated, practical usefulness of the doped GaMnAs is limited by their Curie temperatures which currently<br />
lie below 300K. From this point of view, recently, ZnO based materials have been of growing interest following the<br />
first report [Sharma, P et al., Nature Mater.2, 673 (2003) with over 330 citations it is now the most cited paper from<br />
Nature Materials at present) of room temperature ferromagnetism in Mn doped ZnO thin films. With a band gap in<br />
the ultraviolet at 3.4 eV, ZnO based materials open up a variety of potential applications, especially for spinoptoelectronics,<br />
some of which already exist but currently independent of the spin considerations. Mn 2 + ion has the<br />
largest magnetic moment, 5 μ B, but often the moments measured experimentally have been rather small although the<br />
Tc’s have been above room temperature. Because the properties of ZnO are extremely sensitive to processing<br />
conditions, and the additional fact that Mn has many allotropes of oxides that are magnetic, it was shown by Sharma<br />
et al that the key to obtain above room temperature ferromagnetism is the deposition and processing at temperatures<br />
below 400 o C in a controlled atmosphere. These results have now been extensively reproduced often with<br />
considerably larger magnetic moments per Mn atom. Gamelin and his coworkers found that although the ‘as<br />
obtained’ nanocrystals produced by the colloidal approach were paramagnetic at room temperature, the films<br />
obtained by spincoating on to fused silica with a 2 min aerobic anneal at 500 o C became ferromagnetic with Tc above<br />
RT. In a subsequent experiment (JACS 127, 5292 (2005); PRL 94, 147209 (2005) they also showed that on<br />
Nitrogen-capping the colloidal particles during the processing of the thin films, gave a strong evidence for<br />
ferromagnetism with Mn in 2+ state, while on O-capping it was paramagnetic at room temperature. This result<br />
supports the prediction expected from a theoretical approach that the ferromagnetic order is carrier induced, and is<br />
via the holes in the p-state of ZnO. However, there are many recent experiments which evidence that, although<br />
carrier mediated, ferromagnetic order above RT is also obtained on n-type doping [Narayan et al APL 88, 242503<br />
(2006)]. Another strong evidence for ferromagnetism in Mn doped ZnO is the significant magnetic circular<br />
dischroism at the ZnO band edge observed at room temperature. Along with such a result on doping ZnO with other<br />
TM elements it implies that ferromagnetism is an intrinsic property of the bulk ZnO lattice.(Neal et al PRL 96,<br />
197208 (2006). Neal et al also observed that the MCD data at the ZnO band edge shows room temperature hysteretic<br />
behaviour.<br />
Recently, room temperature ferromagnetism in Mn doped ZnO has also been reported in nanorods, and<br />
freestanding single crystal nanowires, [e.g. APL 88, 263101 (2006)]. All the above facts and many more recent<br />
studies only confirm that we have robust ferromagnetism in Mn doped ZnO at room temperature and can be<br />
exploited for spintronic applications because of its high intrinsic Mn moment. Another challenging support and<br />
promise for device application comes from a recent observation that on Al co-doping Mn doped ZnO, Xu, X.H. et al<br />
[New J. Phys 8, 135 (2006)] obtained in their samples the full moment of Mn and in addition co-doping of Al<br />
resulted in n-type ZnO matrix. This is a significant observation, because we can now think of designing<br />
ferromagnetic n-p junctions at room temperature! Needless to stay that such an electronic element would not be<br />
possible with doped GaMnAs materials.<br />
It is always of interest to look for new and less complex materials suitable for applications in spintronics. In this<br />
context I will also present some highlights of our extensive studies of Room Temperature Ferromagnetism in<br />
semiconductors like ZnO, GaP, GaN In2O3.. doped with non-magnetic elements like Cu, V, Ti, Cr to mention a few<br />
among many others. Theoretical calculations based on the density functional theory (DFT) suggest that the most<br />
stable compounds of Tm(V, Cr Fe, and Ti) doped In 2 O 3 are all ferromagnetic at room temperature and specially in<br />
the case of V doping it gives rise to a rather strong ferromagnetic coupling, and the moment at the V site for example<br />
can be as large 2μ B The magnetic interactions are believed to be mediated by the hybridization between d-states of<br />
V and p-bands of oxygen. In Stockholm we have fabricated Cu doped ZnO films into patterned MRAM type<br />
structures with the patterned elements of size ranging from microns to nanometer scale by using ink-jet printing<br />
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