Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Halbleiterphysik Montag<br />
ture with an electron density of about 10 11 cm −2 and a high mobility of<br />
∼ 10 6 cm 2 V −1 s −1 . A high reflectance AlGaAs/AlAs Bragg mirror below<br />
the 2DEG together with the reflecting top layer of the sample constitute<br />
a cavity around the optical active quantum well. Simulations of the<br />
expected optical Faraday-signal in reflection geometry exhibit a signal enhancement<br />
of almost one order of magnitude due to the presence of the<br />
mirror. Using a Hall bar, we observe the integer quantum-Hall-effect and<br />
Shubnikov-de Haas-oscillations in a magnetic field up to 8 T at a temperature<br />
of 1.8 K. Time-resolved photoluminescence (PL) experiments using<br />
a streak camera system yield electron and hole spin dynamics inside the<br />
quantum well. Simultaneous PL and transport measurements at different<br />
filling factors will be presented.<br />
HL 12.48 Mo 16:30 Poster A<br />
Terahertz Photoleitungs- und Transmissionsspektroskopie an<br />
tunnelgekoppelten doppellagigen zweidimensionalen Elektronengasen<br />
— •L. H. Böttger, S. Holland, C.-M. Hu, Ch. Heyn<br />
und D. Heitmann — Institut für Angewandte Physik, Universität Hamburg<br />
Es wurden spektral aufgelöste Photoleitungs- und Transmissionsmessungen<br />
im Terahertzbereich an einem tunnelgekoppelten GaAs/AlGaAs<br />
Doppelquantentopf durchgeführt. Auf die Probe wurde ein Mäander-<br />
Hallbar mit einer Breite von 50µm und einer Länge von etwa 13cm<br />
präpariert. Ein Gitterkoppler aus Gold mit einer Periode von 1µm bedeckt<br />
den Hallbar, so dass die Goldstreifen senkrecht zum Rand über<br />
den Kanal laufen. Der Versuchsaufbau bestand aus einem Fourierspektrometer,<br />
das mit einem Waveguide mit einem Magnet-Kryostaten verbunden<br />
war. Die Probe wurde in Magnetfeldern von 0 bis 12T bei einer<br />
Temperatur von 1.8K gemessen. Es wurde sowohl in Photoleitung<br />
als auch in Transmission die Zyklotronresonanz und ein Magnetoplasmon<br />
über nahezu den gesamten Magnetfeldbereich beobachtet. Ein Vergleich<br />
der Moden-Energien aus beiden Messmethoden zeigte eine gute<br />
Übereinstimmung bei ganzzahligen Füllfaktoren (ν=2,3,...). Zwischen<br />
den Füllfaktoren jedoch verschob sich die Zyklotronresonanz in den Photoleitungsmessungen<br />
zu höheren Energien während die Magnetoplasmonmode<br />
stark gedämpft wurde.<br />
HL 12.49 Mo 16:30 Poster A<br />
Breakdown of the quantum Hall effect in samples with intentionally<br />
introduced defects — •Dorina Diaconescu, Sascha<br />
Hoch, Dirk Reuter, and Andreas Wieck — Lehrstuhl für Angewandte<br />
Festkörperphysik, Ruhr-Universität Bochum, Germany<br />
We study the role of electron scattering on the onset of the quantum<br />
Hall effect breakdown in 2-dimensional electron systems with intentionally<br />
introduced defects. The defects are Ga ions or vacancies in the<br />
crystal lattice introduced by focused ion beam (FIB) implantation. The<br />
defects can be introduced lateral homogenously, over the whole area of<br />
the Hall-bar, or with spatial resolution. The dependence of the breakdown<br />
current as a function of defect density was investigated in samples<br />
with a lateral homogenous implantation. For low implantation doses, the<br />
critical current increases with the ion dose. Further increase of the ion<br />
dose leads to a reduction of the critical current. The results confirm the<br />
work of Nachtwei et al. [1], where antidot arrays have been patterned on<br />
the GaAs/AlxGa1−xAs heterostucture. The initial increase of the critical<br />
current with the ion dose can be explained by an increased inelastic<br />
scattering rate at the defects. It results a more effective cooling of the<br />
hot electrons. Higher defect densities increase the impurity-assisted inter-<br />
Landau level transitions, and a significant decrease of the critical current<br />
is observed.<br />
[1] G.Nachtwei, G.Lütjering, D.Weiss, Z.H.Liu, K.von.Klitzing, and<br />
C.T.Foxton, Phys.Rev.B.55, 6731 (1996).<br />
HL 12.50 Mo 16:30 Poster A<br />
Strong increase of the electron effective mass in GaAs incorporating<br />
boron and indium — •Tino Hofmann 1 , Claas von<br />
Middendorff 1 , Gunnar Leibiger 2 , Volker Gottschalch 2 , and<br />
Mathias Schubert 1 — 1 Fakultät für Physik und Geowissenschaften,<br />
Institut für Experimentelle Physik II, Universität Leipzig, Linnéstraße<br />
5, 04103 Leipzig — 2 Fakultät für Chemie und Mineralogie, Halbleiterchemie,<br />
Universität Leipzig, Linnéstraße 3, 04103 Leipzig<br />
The strain-free boron- and indium-containing GaAs compounds are<br />
promising candidates for novel III-V semiconductor solar cell absorber<br />
materials with lattice match to GaAs, for which experimental data of the<br />
electronic band structure are widely unknown. We employ far-infrared<br />
magnetooptic ellipsometry to determine the electron effective mass in<br />
non-degenerate, silicon-doped, n-type B0.03In0.06Ga0.91As with a electron<br />
concentration ranging from 2·10 17 to ∼ 1 · 10 18 cm −3 and observe a strong<br />
increase of the electron effective mass of 44% in B0.03In0.06Ga0.91As compared<br />
to In0.06Ga0.94As. Further we report on the vibrational lattice mode<br />
behavior of this quaternary alloy. For BAs, an experimentally obscure<br />
compound, the curvature of the same conduction band extrapolates to<br />
the free electron mass.<br />
HL 12.51 Mo 16:30 Poster A<br />
Optical spectroscopy of perovskitic oxynitrides — •M.<br />
Güngerich 1 , P.J. Klar 1 , W. Heimbrodt 1 , A. Jayakar 2 ,<br />
A. Weidenkaff 2 , S. Ebbinghaus 2 , and A. Reller 2 — 1 FB<br />
Physik und WZMW, Philipps-Universität, Marburg — 2 Lehrstuhl für<br />
Festkörperchemie, Universität Augsburg, Augsburg<br />
Substitution of O by N in mixed metal oxide perovskites are possible<br />
candidates for novel colour pigments. Several different oxynitrides with<br />
ABO3 perovskite structure have been synthesized. Raman spectroscopy<br />
was employed to investigate structural changes taking place when annealing<br />
in air or nitrogen atmosphere. For samples annealed in air, Raman<br />
signals from different types of intermediate states occur in the transition<br />
from the oxynitrides to the corresponding oxides depending on the<br />
type of cations in the crystal. In all the investigated compounds N2 entities<br />
in the crystal lattices were identified by a sharp Raman feature<br />
at 2330cm −1 after heating at temperatures ranging from 500 to 800 ◦ C.<br />
Raman spectra of the untreated and of the partially annealed oxynitrides<br />
show significantly broader signals than the oxides after annealing<br />
at approx. 900 ◦ C. A possible explanation is that the crystalline order is<br />
strongly increased after the full transition of the oxynitrides to the oxides.<br />
Reflectance measurements of single crystals were performed to gain<br />
insight into the correlations between band structure changes and visible<br />
colour changes during the transition from oxides to oxynitrides.<br />
HL 12.52 Mo 16:30 Poster A<br />
Controlled fabrication of well-aligned single-crystalline ZnO<br />
nanowires — •Hongjin Fan, Florian M. Kolb, Roland Scholz,<br />
Margit Zacharias, and Ulrich Gösele — Max-Planck-Institute of<br />
Microstructure Physics, Weinberg 2, 06120 Halle, Germany<br />
Fabrication of ZnO nanowires with controlled morphology, size, and<br />
orientation is essential for their applications in room-temperature UV<br />
nanolasers. By using a vapor transport and condensation process based<br />
on vapor-liquid-solid (VLS) mechanism, ZnO nanowire arrays were successfully<br />
synthesized on sapphire substrates. Electron microscopy investigations<br />
show that the nanowires are aligned mainly vertical to the<br />
sapphire substrate, having heights up to 8 µm and diameters of 30–<br />
150 nm. The nanowires were identified to be single-crystalline hexagonal<br />
wurtzite ZnO and unidirectioned along 〈0001〉. They are structurally uniform<br />
without observable dislocations or an amorphous sheath. In order<br />
to tune the diameter and length of the nanowires, the thickness of the<br />
catalyst Au film and growth time were varied respectively. In addition,<br />
when the Au particles on the substrate were predefined, the position<br />
and density of the ZnO nanowire arrays can be subsequently controlled.<br />
Room-temperature photoluminescence measurements show a sharp UV<br />
emission peak near the band gap of ZnO at 3.36 eV, and a very broad<br />
green emission associated with ionized oxygen vacancy defects.<br />
HL 12.53 Mo 16:30 Poster A<br />
Influence of Bi doping upon the phase change characteristics<br />
of Ge2Sb2Te5 — •Ke Wang, Daniel Wamwangi, and Matthias<br />
Wuttig — I. Physikalisches Institut IA, RWTH Aachen, 52056 Aachen<br />
Ge2Sb2Te5 is a material which is commonly used in rewritable optical<br />
data storage. In this recording technology, the Ge-Sb-Te based alloys have<br />
been successfully developed as commercial products for PD and DVD-<br />
RAM applications due to their relatively short erasing time (30 100ns<br />
for Ge-Sb-Te). To ensure the future success of phase change recording<br />
the data transfer rate needs to be improved further. To achieve this goal<br />
faster materials are required. To this end doping of Ge2Sb2Te5 has been<br />
suggested. Here we report on the influence of Bi doping on the speed<br />
of recrystallization (erasing) process, which is the time limiting step in<br />
optical recording. These experiments were performed by using both a<br />
static tester and an atomic force microscope. The evolution of bit topography<br />
and optical reflectivity under the irradiation of the erasing laser<br />
with different pulse duration is presented. For this Bi doped Ge2Sb2Te5<br />
film, ultrafast erasing is demonstrated and a second amorphization phenomenon<br />
is found during the erasing process. This behavior is related to<br />
structural properties and the activation barrier for the structure transi-