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Plenarvorträge - DPG-Tagungen

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Halbleiterphysik Donnerstag<br />

HL 36 Quantenpunkte und -drähte: Optische Eigenschaften I<br />

Zeit: Donnerstag 10:15–13:30 Raum: H17<br />

HL 36.1 Do 10:15 H17<br />

Structural Relaxation and the Optical Properties of Ge and<br />

Si Nanocrystals – ab initio Calculations — •Weißker Hans-<br />

Christian 1 , Giancarlo Cappellini 2 , Jürgen Furthmüller 1 ,<br />

and Friedhelm Bechstedt 1 — 1 IFTO, Friedrich-Schiller-Universität<br />

Jena, Max-Wien-Platz 1, 07743 Jena — 2 Universitá di Cagliari, Cittadella<br />

Universitaria, Strada Prov.le Monserrato-Sestu, Km 0.700, Italy<br />

Though much effort has been put into the description of the properties<br />

of nanocrystals, ab initio calculations of such systems are still a demanding<br />

task. The ionic degrees of freedom, i.e., the structural relaxation, have<br />

only recently become amenable to ab initio methods for larger clusters<br />

because of the large computational requirements. The use of ultrasoft<br />

pseudopotentials and of the projector-augmented-wave method helps to<br />

alleviate this problem. Size-dependent electron-hole pair excitation energies<br />

calculated by means of a DSCF method are presented.<br />

The ionic relaxation is a twofold problem. First, there is the technical<br />

problem of finding reasonable model structures for the crystallites. This<br />

involves the question of the influence of the ground-state structural relaxation<br />

on the desired quantities. For the optical properties, we demonstrate<br />

that a proper account of the relaxation effects is indispensable<br />

for the quantitative, and in some cases even the qualitative, description.<br />

The second problem is the structural relaxation after electronic excitation,<br />

which results in a contribution of a single nanocrystal to the Stokes<br />

shift measurable for an experimental sample. Model calculations of the<br />

Stokes shift are presented and discussed.<br />

HL 36.2 Do 10:30 H17<br />

Dephasing in Quantum Dots: Quadratic Coupling to Acoustic<br />

Phonons — •Egor Muljarov 1,2 , Frank Grosse 1 , and Roland<br />

Zimmermann 1 — 1 Institut für Physik der Humboldt-Universität zu<br />

Berlin, Newtonstr. 15, 12489 Berlin, Germany — 2 General Physics Institute<br />

RAS, Vavilova 38, Moscow 119991, Russia<br />

A microscopic theory of optical transitions in quantum dots with<br />

carrier-phonon interaction is developed. Virtual transitions into higher<br />

confined states with acoustic phonon assistance add a quadratic phonon<br />

coupling to the standard linear one, thus extending the independent Boson<br />

model. Summing infinitely many diagrams in the cumulant, an exact<br />

solution for the interband polarization is found. Its full time dependence<br />

and the absorption lineshape of the quantum dot are calculated.<br />

A temperature-dependent broadening of the zero-phonon line is obtained<br />

and compared with available experimental data.<br />

HL 36.3 Do 10:45 H17<br />

Investigation of the coupling-dependence on the dephasing in<br />

coupled quantum dots — •Matthias Schwab 1 , P. Borri 1 , W.<br />

Langbein 1 , U. Woggon 1 , M. Bayer 1 , S. Fafard 2 , Z. Wasilewski 2 ,<br />

and P. Hawrylak 2 — 1 Experimentelle Physik II, Otto-Hahn Strasse 4,<br />

44221 Dortmund, Germany — 2 Institute for Microstructural Science, National<br />

Research Concil, Ottawa, K1A 0R6, Canada<br />

Due to their atom-like density of states semiconductor quantum dots<br />

(QD) are often referred to as artificial atoms. QDs receive a lot of attention<br />

as they are possible candidates in the field of quantum information<br />

and cryptography. By shrinking the distance between two QDs, one can<br />

bring the single-particle wave function to an overlap creating so called<br />

semiconductor quantum dot molecules.<br />

A prerequisite for any application of their quantum mechanical properties<br />

is a detailed knowledge of their electronic levels and their coupling<br />

to the environment.<br />

In this talk we report on measurements of the dephasing times of the<br />

exciton in InAs/GaAs quantum dot molecules having different interdot<br />

barrier thicknesses. A heterodyne four-wave-mixing (FWM) technique is<br />

used to measure the dephasing times in a temperature range from 5 K to<br />

60 K. The results are compared to a quantum dot single layer. Systematic<br />

dependencies of the homogeneous linewidth on barrier thickness and on<br />

the temperature are reported.<br />

HL 36.4 Do 11:00 H17<br />

Structure Dependent Few-particle Effects in InAs Quantum<br />

Dots — •Andrei Schliwa, Sven Rodt, Florian Guffarth,<br />

Robert Heitz, Robert Seguin, and Dieter Bimberg — Institut<br />

für Festkörperphysik, Technische Universität Berlin<br />

Interaction between strongly localized charge carriers in zerodimensional<br />

systems like quantum dots (QDs) depend sensitively on<br />

their geometrical properties. Few-particle properties, like the biexciton<br />

binding energies, may vary not only in size but also in sign. Based on<br />

the configuration interaction method those properties are calculated<br />

for realistic InAs QDs as function of their structural properties. The<br />

wavefunctions are obtained from eight-band k·p calculations including<br />

strain and piezoelectric effects.<br />

The problem of correlating calculated and measured spectra can be circumvented<br />

exploiting the monolayer splitting in photoluminescence (PL)<br />

-spectra in appropriately grown samples. Detailed analysis of those spectra<br />

shows that (i) the QDs are very flat, (ii) the QDs have well-defined<br />

interfaces and (iii) each peak represents a subensemble of QDs sharing<br />

the same height. With decreasing transition energy the height of the related<br />

QD-ensemble increases subsequently by one monolayer. Single dot<br />

spectra revealing details of few-particle effects are obtained by cathodoluminescence<br />

measurements with shadow masks. Transition from positive<br />

to negative biexciton binding energy with increasing exciton energy due<br />

to decreasing dot size is observed and understood in the framework of<br />

the above theory.<br />

HL 36.5 Do 11:15 H17<br />

Coulomb effects in the optical spectra of semiconductor quantum<br />

dots — •Norman Baer, Paul Gartner, and Frank Jahnke<br />

— Institute for Theoretical Physics, University Bremen<br />

Emission spectra of individual self-assembeld quantum dots show a rich<br />

structure due to Coulomb correlated multi-exciton states. We present a<br />

theoretical investigation of this system based on a full diagonalisation<br />

scheme for the localized states. In addition to a discussion of the renormalized<br />

electronic energies this procedure allows a direct calculation of<br />

the optical spectra in terms of the Coulomb correlated states.<br />

The resulting multi-exciton spectra are discussed and a simplified<br />

Hamiltonian is introduced in order to explain the main features of the<br />

emission spectra. This simplified Hamiltonian, which is based on the relative<br />

importance of the interaction matrix elements, provides an intuitive<br />

picture for the structure of the multi-exciton emission spectra.<br />

In addition to the spectra resulting from neutral excitons the emission<br />

spectra of excitons in the presence of spectator charges will be discussed.<br />

HL 36.6 Do 11:30 H17<br />

Many-body theory of carrier capture and relaxation in semiconductor<br />

quantum-dot lasers — •Torben Roland Nielsen, Paul<br />

Gartner, and Frank Jahnke — Institute for Theoretical Physics,<br />

University of Bremen, 28334 Bremen, Germany<br />

In quantum-dot laser devices containing a quasi two-dimensional wetting<br />

layer, a pump process initially populates the letting-layer states. The<br />

scattering of carriers from these spatially-extended quasi two-dimensional<br />

states into the quantum-dot states as well as the relaxation of carriers<br />

between the quantum-dot levels are studied theoretically.<br />

Based on the wave functions for the coupled quantum-dot/wettinglayer<br />

system interaction matrix elements are calculated for carrier-carrier<br />

Coulomb interaction and carrier-phonon interaction. Scattering rates<br />

for various capture and relaxation processes are evaluated under quasiequilibrium<br />

conditions.<br />

For elevated carrier densities in the wetting layer, Coulomb scattering<br />

provides processes with capture (relaxation) times typically faster<br />

than 10ps (1ps). When energy conservation allows for interaction with<br />

LO-phonons, comparable rates are obtained.<br />

HL 36.7 Do 11:45 H17<br />

Optical properties of semiconductor microcavity pillars — •J.<br />

Wiersig 1 , N. Baer 1 , P. Gartner 1 , F. Jahnke 1 , M. Benyoucef<br />

2 , S.M. Ulrich 2 und P. Michler 2 — 1 Universität Bremen —<br />

2 Universität Stuttgart<br />

A recent experiment demonstrated the generation of triggered photon<br />

pairs due to cascaded biexciton-exciton emission from a single In-<br />

GaAs/GaAs quantum dot in a cylindrical micropillar [1]. Such experiments<br />

are based on the altered spontaneous emission of carriers in the<br />

microcavity as well as on the selection of optical transitions by the resonator.<br />

Within a detailed theory-experiment comparison we study op-

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