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Book of abstracts - Euro-MBE 2011 - CNRS

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Mo2.1<br />

<strong>MBE</strong> growth <strong>of</strong> LiMnAs<br />

Vít Novák<br />

Institute <strong>of</strong> Physics <strong>of</strong> the Academy <strong>of</strong> Sciences, Cukrovarnická 10, 162 53 Praha, Czech Republic<br />

Compound semiconductors derived from silicon have had a tremendous impact on the physics and<br />

applications <strong>of</strong> semiconductors. Two textbook examples are the direct gap III-V semiconductors and<br />

the prototype magnetic II-VI semiconductors, Fig.1. Remarkably, none <strong>of</strong> the other closest relatives <strong>of</strong><br />

silicon from the I-III-IV and I-II-V compounds have so far been synthesized by modern epitaxial<br />

growth techniques and the potential <strong>of</strong> these compounds has remained virtually unexplored. In this<br />

talk we focus on I-Mn-V compounds which surprisingly have not previously been considered as<br />

candidate semiconductors. One <strong>of</strong> the key motivations to establish their semiconducting electronic<br />

structure is that they are among the rare known silicon relatives with magnetic ordering temperature<br />

safely above room temperature.<br />

Fig.1: Closest relatives <strong>of</strong> silicon emerging by applying the “proton transfer” rule.<br />

We demonstrate on LiMnAs that high-quality materials with group-I alkali metals in the crystal structure<br />

can be grown by standard solid source molecular beam epitaxy [1]. The epitaxial LiMnAs film exhibits<br />

optical gap, evidenced by optical transmission measurements and consistent with the band structure<br />

obtained by our ab initio calculations. Squid magnetometry measurements support earlier reports <strong>of</strong><br />

high antiferromagnetic ordering temperature.<br />

We propose a strategy for employing I-Mn-V compounds in high-temperature semiconductor<br />

magneto-electronics. The key principle is to utilize relativistic magnetic and magneto-transport anisotropy<br />

effects whose common characteristics is that they are an even function <strong>of</strong> the microscopic magnetic<br />

moment vector and are therefore in principle equally well present in materials with ferromagnetic (FM) and<br />

antiferromagnetic (AFM) order. The application <strong>of</strong> AFM semiconductors to exchange bias FMs opens an<br />

immediate research opportunity for integrating conventional semiconductor micro and opto-electronics<br />

functionalities directly in the exchange-biasing AFM layers in common magneto-electronic devices. In<br />

these structures LiMnAs can be combined, e.g., with lattice matched FM semiconductor (In,Mn)As or<br />

conventional transition metal FMs. The FM-AFM coupling can also be used for controlling the staggered<br />

moment orientation in the AFM by the exchange spring effect induced by rotating moments in the<br />

ferromagnet.<br />

[1] T. Jungwirth, et al., Phys. Rev. B 83, 035321 (<strong>2011</strong>).<br />

_______________________<br />

* Contact: vit.novak@fzu.cz

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