Demonstration of molecular beam epitaxy and a semiconducting band structure for I-Mn-V compounds
Authors
T. Jungwirth, V. Novák, X. Martí, M. Cukr, F. Máca, A. B. Shick, J. Mašek, P. Horodyská, P. Němec, V. Holý, J. Zemek, P. Kužel, I. Němec, B. L. Gallagher, R. P. Campion, C. T. Foxon, and J. Wunderlich: Demonstration of molecular beam epitaxy and a semiconducting band structure for I-Mn-V compounds, Phys. Rev. B 83, 035321 (2011).
Our ab initio theory calculations predict a semiconducting band structure of I-Mn-V compounds. We demonstrate on LiMnAs that high-quality materials with group-I alkali metals in the crystal structure can be grown by molecular beam epitaxy. Optical measurements on the LiMnAs epilayers are consistent with the theoretical electronic structure…
Our ab initio theory calculations predict a semiconducting band structure of I-Mn-V compounds. We demonstrate on LiMnAs that high-quality materials with group-I alkali metals in the crystal structure can be grown by molecular beam epitaxy. Optical measurements on the LiMnAs epilayers are consistent with the theoretical electronic structure. Our calculations also reproduce earlier reports of high antiferromagnetic ordering temperature and predict large, spin-orbit-coupling-induced magnetic anisotropy effects. We propose a strategy for employing antiferromagnetic semiconductors in high-temperature semiconductor spintronics [1].
Description
Fig 1. Two branches of the closest relatives of silicon emerging from the
"proton transfer" rule. The left-hand branch is obtained by
imagining one or two proton transfer from the first to
the second atom of the primitive cell; the right-hand branch assumes
that one proton is transferred into an empty interstitial space in the
lattice. Owing to its isovalent nature, Mn naturally extends the
elements from the group-II zinc column.
Description
Fig 2. RHEED image of the LiMnAs film after 60 min of MBE growth.
The lines yield evidence
of the two-dimensional growth character an expected in-plane
crystal symmetry.
Description
Fig 3. Fabry-Pérot interference oscillations of the light back-reflected
by the growing LiMnAs film on an InAs substrate plotted as a function of
the growth time and wavelength of the detected light. The oscillatory
interferences are typical of a semiconductor film.