Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Halbleiterphysik Montag<br />
sed. Phenomena such as coherent suppression of tunnelling in absence<br />
of accidental degeneration of the quasienergies, low-frequency generation<br />
and half harmonic generation are observed. A simplified analytical model<br />
that reproduces the main features of the numerical calculations is presented<br />
and is utilized to derive simple relations for the values of the pulse<br />
parameters that optimize the control process of the electron motion and<br />
its emission spectrum.<br />
HL 12.21 Mo 16:30 Poster A<br />
Photomixing at 1.55µm - Application of the nipnip-THz-emitter<br />
concept to long wavelength materials — •Frank H. Renner 1 , O.<br />
Klar 1 , S. Malzer 1 , M. Eckardt 1 , G. Loata 2 , T. Löffler 2 , H.<br />
Roskos 2 , D. Driscoll 3 , M. Hanson 3 , A.C. Gossard 3 , and G.H.<br />
Döhler 1 — 1 Insitut für Technische Physik I, Universität Erlangen-<br />
Nürnberg , Germany — 2 Lehrstuhl für Ultrakurzzeitphysik, Universität<br />
Frankfurt a.M., Germany — 3 Materials Departement, UC Santa Barbara,<br />
U.S.A.<br />
We have recently developed a novel concept for photomixing based<br />
on the quasi-ballisitic transport of electrons in a nipnip-superlattice. We<br />
were already able to observe THz-radiation from AlGaAs-based samples.<br />
For these samples excitation is performed by photomixing around 830nm<br />
(see oral presentation of our group).<br />
Technologically more favourable would be a photomixer operating<br />
around 1.55µm. Several workgroups are currently trying to find a suitable<br />
photomixer, operating around this wavelength. In this contribution<br />
we extend our nipnip-THz-emitter concept towards 1.55µm by using the<br />
(Al)InGaAs-semiconductor alloy system. Monte Carlo simulations prove<br />
this material system to be substantially superior to AlGaAs. We will discuss<br />
design and concept of the InGaAs-nipnip-emitter, compare it to the<br />
AlGaAs design and report on first results on its realzation.<br />
HL 12.22 Mo 16:30 Poster A<br />
Molecular fluorescence in and near nanostructures — Lavinia<br />
Rogobete 1 , Vahid Sandoghdar 1 , and •Carsten Henkel 2 —<br />
1 Physical Chemistry, ETH Zurich, Switzerland — 2 Institut für Physik,<br />
Universität Potsdam<br />
Single molecular dipoles provide unique opportunities to perform scanning<br />
optical near field microscopy with pointlike sources and detectors.<br />
The electromagnetic interaction with nanostructured probes and with<br />
the scanning tip itself significantly modifies the fluorescence dynamics.<br />
We discuss a simplified, two-dimensional model for the radiative decay<br />
of a single dipole in a complex dielectric or metallic environment [1]. The<br />
electromagnetic fields are computed numerically using boundary integral<br />
equations. The resulting decay rates inside sub-wavelength host particles<br />
compare well with an electrostatic calculation.<br />
[1] Opt. Lett. 28 (2003) 1736.<br />
HL 12.23 Mo 16:30 Poster A<br />
Optical superlattices based on surface acoustic waves — •M. M.<br />
de Lima, Jr., R. Hey, and P. V. Santos — Paul-Drude-Institut,<br />
Berlin<br />
We present a novel concept for the fabrication of dynamic optical superlattices<br />
based on the modulation of a planar photonic microresonator<br />
by surface acoustic waves (SAWs). The microresonator consists of a λ/4<br />
GaAs cavity layer sandwiched between GaAs/AlAs Bragg reflectors. The<br />
optical superlattice is formed by SAW beams, which laterally modulate<br />
the cavity optical properties. The strong light field in the cavity layer<br />
considerably enhances the acousto-optic interaction, thus leading to high<br />
diffraction intensities. We report the observation of stop bands in the light<br />
dispersion as wide as 1.4 meV induced by the lateral periodicity imposed<br />
by the SAWs. We also demonstrate the formation of two-dimensional<br />
superlattices by the interference of orthogonal SAW beams.<br />
HL 12.24 Mo 16:30 Poster A<br />
Emission stimulation in opals — •Sergei Romanov 1 , Dmitry<br />
Chigrin 1 , Clivia Sotomayor Torres 1 , Nikolai Gaponik 2 , Alexander<br />
Eychmueller 2 und Andrei Rogach 3 — 1 Inst. of Materials<br />
Science and Dept. of Electrical and Information Engineering, University<br />
of Wuppertal, 42097, Germany — 2 Inst. of Physical Chemistry, University<br />
of Hamburg, 20146, Germany — 3 Dept. of Physics, University of<br />
Munich, 80799, Germany<br />
Light sources in photonic crystals (PhCs) attract considerable attention<br />
owing to improvement of emitter parameters. We studied the ballistic<br />
emission of CdTe nanocrystals, which were layer-by-layer embedded in<br />
thin opal films, near the Bragg PBG as a function of excitation power<br />
and angle of detection. Two-parameter exponential fit to the emission<br />
intensity vs. excitation power curve was used to extract the power radiated<br />
by saturated emitter and the saturation threshold. In the PBG the<br />
spectrum of the former shows a minimum in contrast to the maximum of<br />
the latter. The decrease of the saturated emission power was associated<br />
with the suppression of the spontaneous emission rate in a given optical<br />
mode and the increase the saturation threshold - as the acceleration of<br />
the radiative recombination.<br />
We argue that photons emitted along the bandgap direction are coupled<br />
to highly inhomogeneous PhC eigenmodes propagating with low<br />
group velocity. This imposes resonator conditions and the backreaction<br />
of the radiation to emitters stimulates the radiative recombination.<br />
HL 12.25 Mo 16:30 Poster A<br />
Light scattering in thin opal films — •Sergei Romanov — Institute<br />
of Materials Science and Department of Electrical and Information<br />
Engineering, University of Wuppertal, 42097 Wuppertal, Germany<br />
Reflectance and transmission are conventionally used to measure light<br />
interaction with photonic crystals (PhCs), whereas the light scattered<br />
off the incidence direction is neglected. In this work the scattering was<br />
used as an independent tool to study the light propagation in slightly<br />
disordered three-dimensional PhCs. In such crystals the regime of weak<br />
scattering is realised, when scattered photons experience only one collision<br />
along their paths, i.e. they mimic light emitted by an internal light<br />
source.<br />
The intensity of light scattered by thin opal films in forward and backward<br />
configurations was studied as a function of wavelength and direction.<br />
It was shown that diffraction-related minima of forward scattered<br />
light do not depend on the actual lightpath, but correspond to directions<br />
of the incidence and detection with respect to (111) planes. Angle diagrams<br />
of the scattered light were assigned to the resonant scattering,<br />
moreover, they show a modulation by shadows of respective bandgaps.<br />
Oppositely, the backscattering appears more effective at bandedges of<br />
the Bragg gap.<br />
As an example, the light scattering was used to characterise the light<br />
propagation across the PhC heterojunction.<br />
HL 12.26 Mo 16:30 Poster A<br />
Asymptotic analysis of radiation pattern of a classical dipole in<br />
a photonic crystal — •Dmitry Chigrin and Clivia Sotomayor<br />
Torres — Institute of Materials Science and Department of Electrical,<br />
Information and Media Engineering, University of Wuppertal, D-42097<br />
Wuppertal, Germany<br />
Photonic crystals (PhCs) possess a complicated photonic band structure,<br />
where allowed bands display strong dispersion and anisotropy. Recently,<br />
there has been a growing interest in studies of energy flow inside<br />
PhCs. Being a strongly anisotropic material, a PhC displays the beam<br />
steering effect: the group velocity direction does not necessarily coincide<br />
with the wavevector direction. As a consequence, the emission of an optically<br />
active material placed within a PhC can reveal unusual properties.<br />
In this contribution, an asymptotic analysis of the electromagnetic<br />
field of a classical point dipole situated in PhC possessing an incomplete<br />
bandgap is presented. The simple formula to calculate an angular distribution<br />
of radiated power is introduced. Redistribution of the radiated<br />
power is predicted. Within given approximation, the radiated power becomes<br />
infinite in certain directions. These are directions in which the<br />
direction of the group velocity of the crystal eigenmodes is stationary<br />
with respect to a small variation in the wavevector direction. Predictions<br />
of asymptotic analysis are substantiated with FTDT calculation.<br />
HL 12.27 Mo 16:30 Poster A<br />
Dynamics and entanglement of photon pulses in a photonic<br />
crystal — Geesche Boedecker and •Carsten Henkel — Institut<br />
für Physik, Universität Potsdam<br />
In a photonic crystal, the dispersion relation of light can be tailored to<br />
a great extent. Close to a band edge, for example, the group velocity is<br />
significantly reduced. For a finite crystal slab, multiple reflections from<br />
the end faces lead to a transmitted pulse train. We discuss the entanglement<br />
properties of the transmitted pulses. The pulse shape inside the<br />
crystal is analyzed for a one-dimensional model [1] in the regime of small<br />
group velocities.<br />
[1] Opt. Express 11 (2003) 1590