We report on the epitaxial growth of a group-IV ferromagnetic semiconductor, Mn(x)Ge(1-x), in which the Curie temperature is found to increase linearly with manganese (Mn) concentration from 25 to 116 kelvin. The p-type semiconducting character and hole-mediated exchange permit control of ferromagnetic order through application of a +/-0.5-volt gate voltage, a value compatible with present microelectronic technology. Total-energy calculations within density-functional theory show that the magnetically ordered phase arises from a long-range ferromagnetic interaction that dominates a short-range antiferromagnetic interaction. Calculated spin interactions and percolation theory predict transition temperatures larger than measured, consistent with the observed suppression of magnetically active Mn atoms and hole concentration.
We have fabricated a thin film magnetic system consisting of nanoscale Mn11Ge8 ferromagnetic clusters embedded in a MnxGe1−x dilute ferromagnetic semiconductor matrix. The clusters form for growth temperatures of ∼300 °C with an average diameter and spacing of 100 and 150 nm, respectively. While the clusters dominate the magnetic properties, the matrix plays a subtle but interesting role in determining the transport properties. Variable range hopping at low temperatures involves both nanoclusters and MnGe sites, and is accompanied by a negative magnetoresistance attributed in part to spin-dependent scattering analogous to metallic granular systems.
A Group-IV Ferromagnetic Semiconductor: MnxGe 1−x .-Singlecrystal films of the title compound are grown on Ge and GaAs(001) substrates by molecular beam epitaxy. These films have Curie temperatures in the range 25 to 116 K, are p-type semiconductors, and exhibit a pronounced extraordinary Hall effect. Density functional theory calculations show that the magnetically ordered phase arises from a long-range ferromagnetic interaction that dominates a short-range antiferromagnetic interaction. Calculated spin interactions and percolation theory predict transition temperatures larger than measured, consistent with the observed suppression of magnetically active Mn atoms and hole concentration. The p-type semiconducting character and hole-mediated exchange permit control of ferromagnetic order through application of a gate voltage. -(PARK, Y. D.; HANBICKI, A. T.; ERWIN, S. C.; HELLBERG, C. S.; SULLIVAN, J. M.; MATTSON, J. E.; AMBROSE, T. F.; WILSON, A.; SPANOS, G.; JONKER, B. T.; Science (Washington, D.
An epitaxial orientation of Fe/Cr superlattices -Fe/Cr(211) on MgO(110)is grown by magnetron sputtering.Its structural and magnetic characterizations are presented and compared to those for Fe/Cr(100) superlattices grown simultaneously onto MgO(100) substrates. The epitaxial orientation of the Fe/Cr (211) superlattices is Fe/Cr[011]~iMgO[001] and Fe/Cr[111]iiMgO[110], while that for Fe/Cr(100) is Fe/Cr[001]~~MgO[011]. A uniaxial, in-plane surface anisotropy for the Fe/Cr(211) superlattices along the Fe[011]of 0.06 erg/cm2 is obtained from analysis of the magnetization hysteresis loops.Four oscillations in the antiferromagnetic interlayer coupling and giant magnetoresistance (CiMR) are 0 observed with a period of 18 A for both orientations. The strength, oscillation period, and phase of the magnetic coupling are identical for the two orientations. The GMR values increase by a factor of -4 to 5 on cooling from room temperature to 4.2 K. At 4.2 K the maximum GMR value of the [Fe(14 A)/Cr(8 A)],0 superlattice is 70% for the (211) orientation and 150% for the (100) orientation.
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