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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.

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