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Publication
Featured researches published by G. Schmidt.
Nature | 1999
R. Fiederling; M. Keim; G. Reuscher; W. Ossau; G. Schmidt; A. Waag; L. W. Molenkamp
The field of magnetoelectronics has been growing in practical importance in recent years. For example, devices that harness electronic spin—such as giant-magnetoresistive sensors and magnetoresistive memory cells—are now appearing on the market. In contrast, magnetoelectronic devices based on spin-polarized transport in semiconductors are at a much earlier stage of development, largely because of the lack of an efficient means of injecting spin-polarized charge. Much work has focused on the use of ferromagnetic metallic contacts, but it has proved exceedingly difficult to demonstrate polarized spin injection. More recently, two groups have reported successful spin injection from an NiFe contact, but the observed effects of the spin-polarized transport were quite small (resistance changes of less than 1%). Here we describe a different approach, in which the magnetic semiconductor BexMnyZn1-x-ySe is used as a spin aligner. We achieve injection efficiencies of 90% spin-polarized current into a non-magnetic semiconductor device. The device used in this case is a GaAs/AlGaAs light-emitting diode, and spin polarization is confirmed by the circular polarization state of the emitted light.
Applied Physics Letters | 2001
Th. Gruber; M. Keim; R. Fiederling; G. Reuscher; W. Ossau; G. Schmidt; L. W. Molenkamp; A. Waag
One major challenge for the development of spintronic devices is the control of the spin polarization of an electron current. We propose and demonstrate the use of a BeTe/Zn1−xSe/BeTe double barrier resonant tunneling diode for the injection of a spin-polarized electron current into GaAs and the manipulation of the spin orientation of the injected carriers via an external voltage. A spin polarization of up to 80% can be observed with a semimagnetic layer of only 3.5 nm thickness. By changing the resonance condition via the external voltage, the degree of spin polarization can be varied, though a complete spin switching has not yet been accomplished.
Physical Review Letters | 2006
C. Gould; A. Slobodskyy; D. Supp; T. Slobodskyy; P. Grabs; P. Hawrylak; F. Qu; G. Schmidt; L. W. Molenkamp
A key element in the emergence of a full spintronics technology is the development of voltage controlled spin filters to selectively inject carriers of desired spin into semiconductors. We previously demonstrated a prototype of such a device using a II-VI dilute-magnetic semiconductor quantum well which, however, still required an external magnetic field to generate the level splitting. Recent theory suggests that spin selection may be achievable in II-VI paramagnetic semiconductors without external magnetic field through local carrier mediated ferromagnetic interactions. We present the first experimental observation of such an effect using non-magnetic CdSe self-assembled quantum dots in a paramagnetic (Zn,Be,Mn)Se barrier.
Applied Physics Letters | 2005
G. V. Astakhov; A.V. Kimel; G. M. Schott; Artem Tsvetkov; Andrei Kirilyuk; D. R. Yakovlev; G. Karczewski; W. Ossau; G. Schmidt; L. W. Molenkamp; T.H.M. Rasing
We demonstrate complete reversal of a full magnetic hysteresis loop of the magnetic semiconductor (Ga,Mn)As by ultrashort optical excitation with a single subpicosecond light pulse, with obvious implications for ultrafast magneto-optical recording. Our approach utilizes the fourfold magnetic anisotropy of (Ga,Mn)As, in combination with the magnetic linear dichroism of the material.
Physical Review Letters | 2006
G. V. Astakhov; T. Kiessling; A. V. Platonov; T. Slobodskyy; Suddhasatta Mahapatra; W. Ossau; G. Schmidt; K. Brunner; L. W. Molenkamp
We report circular-to-linear and linear-to-circular conversion of optical polarization by semiconductor quantum dots. The polarization conversion occurs under continuous wave excitation in absence of any magnetic field. The effect originates from quantum interference of linearly and circularly polarized photon states, induced by the natural anisotropic shape of the self assembled dots. The behavior can be qualitatively explained in terms of a pseudospin formalism.
Applied Physics Letters | 2001
L. Hansen; D. Ferrand; G. Richter; M. Thierley; V. Hock; N. Schwarz; G. Reuscher; G. Schmidt; L. W. Molenkamp; A. Waag
We report on the molecular-beam epitaxial growth and magnetotransport properties of p-type BeMnTe, a ferromagnetic diluted magnetic semiconductor. BeMnTe thin-film structures can be grown almost lattice matched to GaAs for Mn concentrations up to 10%. A high p-type doping with nitrogen can be achieved by using a rf plasma source. BeMnTe and BeTe layers have been characterized by magnetotransport measurements. At low temperatures, the BeMnTe samples exhibit a large anomalous Hall effect. A hysteresis in the anomalous Hall effect appears below 2.5 K in the most heavily doped sample, which indicates the occurrence of a ferromagnetic phase.
Applied Physics Letters | 2006
M. K. Kneip; D. R. Yakovlev; M. Bayer; T. Slobodskyy; G. Schmidt; L. W. Molenkamp
We show that the magnetization dynamics in diluted magnetic semiconductors can be controlled separately from the static magnetization by means of an electric field. The spin-lattice relaxation (SLR) time of magnetic Mn2+ ions was tuned by two orders of magnitude by a gate voltage applied to n-type modulation-doped (Zn,Mn)Se∕(Zn,Be)Se quantum wells. The effect is based on providing an additional channel for SLR by a two-dimensional electron gas (2DEG). The static magnetization responsible for the giant Zeeman spin splitting of excitons was not influenced by the 2DEG density.
Physical Review B | 2005
D. Keller; D. R. Yakovlev; G. V. Astakhov; W. Ossau; S. A. Crooker; T. Slobodskyy; A. Waag; G. Schmidt; L. W. Molenkamp
The optical properties of two-dimensional electron gases in
Journal of Superconductivity | 2001
A. Waag; Th. Gruber; G. Reuscher; R. Fiederling; W. Ossau; G. Schmidt; L. W. Molenkamp
mathrm{Zn}mathrm{Se}∕(mathrm{Zn},mathrm{Be})mathrm{Se}
Physical Review B | 2006
T. Kiessling; A. V. Platonov; G. V. Astakhov; T. Slobodskyy; Suddhasatta Mahapatra; W. Ossau; G. Schmidt; K. Brunner; L. W. Molenkamp
and