Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Halbleiterphysik Donnerstag<br />
HL 37 Quantenpunkte und -drähte: Transporteigenschaften<br />
Zeit: Donnerstag 10:15–13:30 Raum: H13<br />
HL 37.1 Do 10:15 H13<br />
Spin Blockade in Capacitively Coupled Quantum Dots — •M.<br />
C. Rogge, C. Fühner, U. F. Keyser, and R. J. Haug — Institut<br />
für Festkörperphysik, Universität Hannover, D-30167 Hannover<br />
We present transport measurements on a lateral double dot produced<br />
by combining local anodic oxidation and electron beam lithography [1].<br />
Our device is based on a GaAs/AlGaAs heterostructure containing a<br />
two-dimensional electron system (2DES) 34 nm below the surface. We<br />
use an atomic force microscope (AFM) to write the basic double dot<br />
structure by local anodic oxidation (LAO) [2]. We complete our device<br />
with a metallic top gate patterned with e-beam lithography to add the<br />
function of controlled tunability of the interdot coupling. We investigate<br />
our device in transport measurements in a 3He/4He dilution refrigerator<br />
and demonstrate, that we can switch between capacitive and tunnel<br />
coupling with top gate voltage. In the regime of capacitive coupling we<br />
focus on the magnetic field dependence in the Coulomb blockade regime.<br />
We observe oscillating peak positions and peak amplitudes for transport<br />
over one dot. This is explained by the phenomenon of spin blockade [3],<br />
which has not been observed in LAO-devices so far. We investigate this<br />
effect and analyze the influence of capacitive interdot coupling in this<br />
regime [4].<br />
[1] M. C. Rogge et al., Appl. Phys. Lett. 83, 1163 (2003)<br />
[2] U. F. Keyser et al., Appl. Phys. Lett. 76, 457 (2000)<br />
[3] M. Ciorga et al., Phys. Rev. B 61, R16315 (2000)<br />
[4] M. C. Rogge et al., cond-mat/0310469 (2003)<br />
HL 37.2 Do 10:30 H13<br />
Wave-function mapping of InAs quantum dots by scanning<br />
tunneling spectroscopy — •Theophilos Maltezopoulos, Arne<br />
Bolz, Christian Meyer, Christian Heyn, Wolfgang Hansen,<br />
Markus Morgenstern, and Roland Wiesendanger — Institute of<br />
Applied Physics, University of Hamburg, Jungiusstr. 11, D-20355 Hamburg,<br />
Germany<br />
Low temperature UHV scanning tunneling spectroscopy is used to investigate<br />
the single-electron states and the corresponding squared wavefunctions<br />
of individual and free-standing strain-induced InAs quantum<br />
dots grown on GaAs(001) by molecular beam epitaxy. Several peaks are<br />
found in dI/dV -curves above the dots, which belong to different singleelectron<br />
states. Spatially resolved dI/dV -images at the peak positions<br />
reveal (000)-, (100)-, (010)-, (200)-, and (300)-states, where the numbers<br />
describe the number of nodes in [110]-, [110]-, and [001]-direction, respectively.<br />
It is found, that the total number and energetic sequence of<br />
states is different for different dots. Additionally, the (010)-state is often<br />
missing, even when (200)- and (300)-states are present. This electronic<br />
anisotropy is attributed to the shape asymmetry of the dots.<br />
HL 37.3 Do 10:45 H13<br />
Direct observation of tunneling escape from InAs/GaAs<br />
quantum dots — •Erik Stock, Martin Geller, Roman Sellin,<br />
and Dieter Bimberg — Technische Universität Berlin, Institut für<br />
Festkörperphysik Hardenbergstr. 35, 10623 Berlin<br />
A major challenge in the investigations of quantum dots (QDs) is to<br />
distinguish between two competing charge carrier emission processes:<br />
thermal activated and tunneling emission [1]. We report here the first<br />
observation of the hole tunneling process via time resolved capacitance<br />
transient spectroscopy (DLTS) measurements at low temperature, where<br />
thermal emission is negligible. The escape time observed by us is independent<br />
from the temperature but strongly depends on the applied reverse<br />
bias, which determines the electric field in the QD layer. The measured<br />
hole tunneling emission time constant is in the order of seconds (for electric<br />
fields of about 100kV/cm), approximately three orders of magnitude<br />
larger than for the ground state tunneling of electrons. The dependence of<br />
the tunneling time constant on the electric field is compared to a model,<br />
assuming a triangular barrier with a potential depth measured directly<br />
by DLTS and photoluminescence excitation (PLE) measurements.<br />
This work was funded by the Nanomat project of the European Commission<br />
Growth Programme, contract number G5RD-CT-2001-00545, Intas<br />
project 2001-774, and SFB 296 of DFG.<br />
[1] C.M.A. Kapteyn et al. Phys. Rev. B 60, (20), 14265 (1999)<br />
HL 37.4 Do 11:00 H13<br />
Spin effects in quantum dots — •Jens Könemann 1 , D. K.<br />
Maude 2 , V. Avrutin 3 , A. Waag 3 , and R. J. Haug 1 — 1 Institut<br />
für Festkörperphysik, Universität Hannover, Appelstrasse 2, D-30167<br />
Hannover, Germany — 2 High Magnetic Field Laboratory, CNRS, 25<br />
Avenue des Martyrs, BP 166, F-38042 Grenoble cedex 9, France —<br />
3 Abteilung Halbleiterphysik, Universität Ulm, Albert-Einstein-Allee<br />
45,D-89069 Ulm, Germany<br />
We present spin-resolved measurements of the transport spectrum of<br />
an individual localized state in a double-barrier resonant tunneling device<br />
probed by single-electron tunneling [1]. We investigated the spin splitting<br />
of ground and excited states and found a deviation to a linear increase<br />
of spin splitting with magnetic field beyond 18 T. Astonishingly, we observed<br />
at high magnetic fields above 14 T a flip of the resonance position<br />
of the energetically higher spin component to a lower energy, whereas the<br />
other spin-component remained unchanged. A hysteresis effect appeared<br />
at the spin flip region as well. Such ”spin-flip”behaviour was observed<br />
on different Fock-Darwin levels, where it occurred at different magnetic<br />
fields. We relate this effect to the presence of magnetic impurities residual<br />
inside the quantum well.<br />
[1] J. Könemann et al., to appear in Physica E<br />
HL 37.5 Do 11:15 H13<br />
Coulomb effects in tunneling through a quantum dot stack — H.<br />
Sprekeler, •G. Kießlich, A. Wacker, and E. Schöll — Institut<br />
für Theoretische Physik, TU Berlin, Hardenbergstr. 36, 10623 Berlin<br />
Resonant tunneling through two vertically coupled self-organized quantum<br />
dots is studied by means of a Pauli master equation model. The<br />
observation of double peaks in the current-voltage characteristic in a recent<br />
experiment [1] as a signature of Coulomb interaction is analyzed in<br />
terms of the tunnel coupling between the quantum dots and the coupling<br />
to the contacts. Different regimes for the emitter chemical potential indicating<br />
different peak scenarios in the tunneling current are discussed. By<br />
comparison with a density matrix approach we show that the interplay<br />
of coherent and incoherent effects in the stationary current can be fully<br />
described by this approach.<br />
[1] M. Borgstrom, T. Bryllert, T. Sass, B. Gustafson, L.-E. Wernersson,<br />
W. Seifert, and L. Samuelson, Appl. Phys. Lett. 78, 3232 (2001)<br />
[2] H. Sprekeler, G. Kießlich, A. Wacker, and E. Schöll, cond-mat/0309696<br />
(unpublished)<br />
HL 37.6 Do 11:30 H13<br />
Fano and Kondo Resonances in Three-Leaded Quantum Dot<br />
Systems — •Armin C. Welker, David Quirion, Juergen Weis<br />
und Klaus v. Klitzing — Max-Planck-Institut fuer Festkoerperforschung,<br />
D -70569 Stuttgart, Heisenbergstr. 1, Germany<br />
The spectral function or density of states of a quantum dot coupled<br />
to two leads can be investigated by weakly coupling a third lead to the<br />
quantum dot. For doing so, the differential conductance to this third lead<br />
is measured as a function of the bias voltage applied to this probing lead<br />
in reference of the two main leads. The feasibility of this approach for<br />
investigating the out-of-equilibrium splitting of the Kondo resonance has<br />
been theoretically explored [1]. We present our preliminary experimental<br />
results on a split-gate quantum dot indicating this splitting.<br />
In addition, measurements on a quantum dot system are shown in the<br />
regime of strong coupling to the two main leads where Fano-like resonances<br />
occur. A peak in the differential conductance to the third lead is<br />
observed whenever a Fano-like resonance is obtained in the conductance<br />
between the two main leads. [1] E. Lebanon and A. Schiller, Phys. Rev.<br />
B 65, 035308 (2002).<br />
HL 37.7 Do 11:45 H13<br />
Hole transport through an array of self-assembled Ge quantum<br />
dots — •Kai-Martin Haendel 1 , U. Denker 2 , O. G. Schmidt 2 ,<br />
and R. J. Haug 1 — 1 Institut für Festkörperphysik, Universität<br />
Hannover, Appelstr. 2, 30167 Hannover — 2 Max-Planck-Institut für<br />
Festkörperforschung, Heisenbergstr. 1, 70569 Stuttgart<br />
In recent years, several features of quantum states in self-assembeld Ge<br />
quantum dots have been demonstrated by various spectroscopic studies,<br />
such as admittance, capacitance-voltage analysis, photoluminescence and<br />
photoluminescence excitation spectroscopy.