Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Halbleiterphysik Freitag<br />
limit is performed.<br />
References: J. Schliemann, J. C. Egues, and D. Loss, Phys. Rev. Lett.<br />
90, 146801 (2003).<br />
J. Schliemann and D. Loss, Phys. Rev. B 68, 165311 (2003).<br />
J. Schliemann and D. Loss, cond-mat/0310108.<br />
HL 49.2 Fr 11:15 H13<br />
Two-dimensional hole precession in an all-semiconductor spin<br />
field effect transistor — •Marco G. Pala 1,2 , Michele Governale<br />
1,3 , Jürgen König 1,4 , Ulrich Zülicke 1,5 , and Giuseppe Iannaccone<br />
2 — 1 Institut für Theoretische Festkörperphysik, Universität<br />
Karlsruhe, Germany — 2 Dipartimento di Ingegneria dell’Informazione,<br />
Università degli Studi di Pisa, Italy — 3 NEST-INFM & Scuola Normale<br />
Superiore, Pisa, Italy — 4 Institut für Theoretische Physik III, Ruhr-<br />
Universität Bochum, Germany — 5 Institute of Fundamental Sciences,<br />
Massey University, New Zealand<br />
We present a theoretical study of a spin field-effect transistor<br />
[1] realized in a quantum well formed in a p–<br />
doped ferromagnetic-semiconductor- nonmagnetic-semiconductorferromagnetic-semiconductor<br />
hybrid structure. Based on an envelopefunction<br />
approach for the hole bands, we derive the full theory of coherent<br />
transport through the device, which includes both heavy- and light-hole<br />
subbands, proper modeling of the mode matching at the interfaces,<br />
integration over injection angles, Rashba spin precession [2], interference<br />
effects due to multiple reflection, and gate-voltage dependence. [1]<br />
S. Datta and B. Das, Appl. Phys. Lett. 56, 665, (1990). [2] E. I. Rashba,<br />
Fiz. Tverd. Tela (Leningrad) 2, 1224 (1960) [Sov. Phys. Solid State 2,<br />
1109 (1960)].<br />
HL 49.3 Fr 11:30 H13<br />
Magnetic moment induced by spin-polarized currents in a<br />
semiconductor heterostructure — •Frank Lehmann, Charles<br />
Gould, Christian Rüster, Peter Grabs, Georg Schmidt, and<br />
Laurens W. Molenkamp — Unversität Würzburg, Physikalisches<br />
Institut (EP 3), Am Hubland, D-97974 Würzburg, Germany<br />
In recent years, several experiments have successfully demonstrated the<br />
electrical injection of spin-polarized currents into semiconductors. These<br />
experiments are sensitive to the polarization of the current but not to the<br />
magnetic moment induced by the spin-polarized carriers. We have now<br />
successfully performed SQUID experiments that provide direct evidence<br />
of a current induced magnetization in an electrical spin injection device.<br />
The magnetic moment of a ZnBeMnSe/GaAs heterostructure was measured<br />
using a SQUID magnetometer and lock-in technique at various<br />
magnetic fields, currents, and temperatures. When the background magnetic<br />
moment that results from Biot-Savart‘s law is eliminated, we observe<br />
a clear change in the magnetic moment at the field and current<br />
configurations for which spin injecton is expected. The field and temperature<br />
dependence show that the effect is related to the magnetization<br />
of the DMS. We interpret our results in terms of (i) the band bending<br />
that occurs in the DMS at higher eletric fields and that reduces the spinpolarization<br />
in the magnetic material and (ii) spin accumulation in the<br />
GaAs.<br />
HL 49.4 Fr 11:45 H13<br />
Positive cross correlations in a three-terminal quantum dot with<br />
ferromagnetic contacts — •Wolfgang Belzig, Audrey Cottet,<br />
and Christoph Bruder — Department für Physik, Universität Basel,<br />
Klingelbergstr. 82, 4056 Basel, Schweiz<br />
We study current fluctuations in a three-terminal quantum dot with<br />
ferromagnetic leads in the sequential tunneling regime. Dynamical spin<br />
blockade on the dot leads to positive zero-frequency cross-correlations of<br />
the currents in the output leads. We include the influence of spin-flip scattering<br />
and identify favorable conditions for the experimental observation<br />
of this effect with respect to polarization of the contacts and tunneling<br />
rates.<br />
HL 50 Quantenpunkte und -drähte: Optische Eigenschaften III<br />
Zeit: Freitag 11:00–13:30 Raum: H14<br />
HL 50.1 Fr 11:00 H14<br />
Optical Detection of Single-Electron Spin Decoherence in<br />
a Quantum Dot — •Oliver Gywat 1 , Hans-Andreas Engel<br />
1 , Daniel Loss 1 , R.J. Epstein 2 , F. Mendoza 2 , and D.D.<br />
Awschalom 2 — 1 Department of Physics and Astronomy, University<br />
of Basel, Switzerland — 2 Center for Spintronics and Quantum<br />
Computation, University of California, Santa Barbara, USA<br />
We propose a method based on optically detected magnetic resonance<br />
(ODMR) to measure the decoherence time T2 of a single electron spin in<br />
a semiconductor quantum dot. The electron spin resonance (ESR) of a<br />
single excess electron on a quantum dot is probed by circularly polarized<br />
laser excitation. Due to Pauli blocking, optical excitation is only possible<br />
for one of the electron spin states. The photoluminescence is modulated<br />
due to the ESR which enables the measurement of electron spin decoherence.<br />
We study different possible schemes for such an ODMR setup.<br />
(cond-mat/0307669)<br />
HL 50.2 Fr 11:15 H14<br />
Optical properties of localized excitons in InGaN quantum<br />
structures — •Til Bartel 1 , Matthias Dworzak 1 , Martin<br />
Strassburg 2 , Axel Hoffmann 1 , Andre Strittmatter 1 , and<br />
Dieter Bimberg 1 — 1 Institut für Festkörperphysik, Technische<br />
Universität Berlin, Hardenbergstr. 36, 10623 Berlin — 2 Georgia State<br />
University, Dep. of Physics and Astronomy, Atlanta, GA-30303<br />
Although InGaN structures already find application in optoelectronics,<br />
its optical transitions are still poorly understood and are subject to<br />
current investigation. Indium fluctuations in InGaN quantum-wells are<br />
centers of localization for excitons and show quantum dot-like behavior<br />
at low temperatures.<br />
Wurzite InGaN/GaN single quantum wells were grown by metal organic<br />
chemical vapor deposition on Si(111) and their luminescence was<br />
investigated. High resolution µ-photoluminescence (µ-PL) spectra of<br />
masked samples showed lines as narrow as the resolution limit. This is<br />
interpreted as an indication for δ-shaped density of states. Excitation<br />
density dependence allows the identification of excitons and biexcitones<br />
with positive and negative binding energies. Time resolved PL experiments<br />
show decay rates of less than 1 ns and investigation of temperature<br />
dependence of the photoluminescence reveal typical S-shape behavior.<br />
These results demonstrate the quantum dot-like character of the indium<br />
fluctuations.<br />
HL 50.3 Fr 11:30 H14<br />
Selective optical charging of self-assembled InGaAs quantum<br />
dots — •Miro Kroutvar, Yann Ducommun, Jon J Finley, Max<br />
Bichler, and Gerhard Abstreiter — Walter Schottky Institut,<br />
Technische Universit”at M”unchen, Am Coulombwall 3, 85748 Garching,<br />
Germany<br />
Charge and spin excitations in individual quantum dots (QDs) have<br />
been proposed as QBITS for implementation of quantum logic. One of<br />
the main challenges for these applications is the selective creation of<br />
electrons in such systems and control of their spin degree of freedom.<br />
We present a QD charging device which enables to optically generate<br />
single charges and potentially spins in sub-ensembles of self-assembled<br />
InGaAs QDs. The device consists of a single layer of InGaAs QDs embedded<br />
within the intrinsic region of a GaAs Schottky photodiode. The<br />
charge storage mechanism relies on selective exciton ionization following<br />
resonant optical generation. Our results demonstrate unambiguously<br />
selective charging with extremely long (¿25 µs) charge storage lifetimes<br />
at low temperatures (10K). Analysis of the energy and temperature dependence<br />
of the charge storage signal permits investigation of the role of<br />
exciton-phonon coupling during the QD resonant absorption process. In<br />
addition, thermally-activated redistribution of resonantly stored charge<br />
among the QD ensemble is identified to be the cause of a time-dependent<br />
loss of spectral selectivity at elevated temperatures. Our storage device<br />
enables to probe directly resonant carrier excitation processes and potentially<br />
electron spin dynamics in micro-ensembles of semiconductor QDs.