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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-

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