Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Halbleiterphysik Dienstag<br />
been recently demonstrated in our laboratory. A challenge lies in the massproduction of 50 m 2 wafers with cost-effective methods.<br />
HL 20 Photonische Kristalle IV<br />
Zeit: Dienstag 15:15–17:30 Raum: H17<br />
HL 20.1 Di 15:15 H17<br />
Optical characterisation of opal heterojunctions — •Sergei<br />
Romanov 1 , Dmitry Chigrin 1 , Vladimir Solovyev 1 , Clivia<br />
Sotomayor Torres 1 , Nikolai Gaponik 2 , Alexander Eychmueller<br />
2 , and Andrei Rogach 3 — 1 Inst. of Materials Science<br />
and Dept. of Electrical and Information Engineering, University of<br />
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 />
Interfacing of photonic crystals (PhCs) is a step towards their functionalisation.<br />
The anticipated effects are engineered PBG, light confinement<br />
and directing of the light flow. Hetero-opals were prepared by sandwiching<br />
two thin film opals assembled from latex beads of different diameters,<br />
while staying with preparation by self-assembly. Angle-resolved<br />
reflectance, transmission, scattering and emission of light were used to<br />
characterise hetero-opals.<br />
Anomalous transmission minimum was observed in between two Bragg<br />
gaps of the hetero-opal constituents and associated with the interface.<br />
This observation was supplemented by reflectance and scattering experiments.<br />
Finite difference time domain modelling of light propagation in<br />
2D PhC hetero-junction was used to study this effect.<br />
Anomalies of emission spectra of CdTe nanoparticles embedded in<br />
hetero-opals, which were observed at frequencies of the interface gap,<br />
agree the interface gap model.<br />
HL 20.2 Di 15:30 H17<br />
EFFECTS OF DISORDER IN MICROWAVE REALI-<br />
ZATIONS OF 1D PHOTONIC CRYSTALS: — •G.A.<br />
Luna-Acosta 1,2 , H. Schanze 1 , U. Kuhl 1 und H.-J. Stöckmann 1<br />
— 1 Fachbereich Physik der Philipps Universität Marburg, Renthof 5,<br />
D-35032 — 2 Instituto de Fisica, BUAP, Puebla, Mexico.<br />
We experimentally investigate the effects of structural and impurity<br />
disorder in 1D photonic lattices and superlattices of finite length. These<br />
lattices are realized in the microwave regime by an array of teflon pieces<br />
of length dT alternating periodically with air spacings of length dA in a<br />
single-mode microwave guide experiment. Structural ( positional) disorder<br />
is achieved by an uncorrelated random variation ξ of the air spacings<br />
and/or the teflon inserts. Impurity disorder is realized by placing a few<br />
teflon pieces of length dimp within the air spacing of the ideal crystal. The<br />
manifestation in the transmission measurements of weak, intermediate,<br />
and strong disorder of both types of disorder is analyzed and compared<br />
with simple transfer matrix calculations. We also discuss our results in<br />
connection with theories of correlated and uncorrelated random disorder<br />
in 1D potentials.<br />
HL 20.3 Di 15:45 H17<br />
Resonant 2D-PC structures of moderate refractive index<br />
materials — •Gunnar Böttger, Markus Schmidt, Karolin<br />
Preusser-Mellert, Alexander Petrov, and Manfred Eich —<br />
Technische Universität Hamburg-Harburg, AB 4-09, 21071 Hamburg<br />
We present simulations and experimental measurements of transmission<br />
properties of photonic crystal slab structures defined by air holes<br />
etched into polymeric slab waveguides. Geometric defects in otherwise<br />
regular photonic crystal slab structures strongly localize optical fields,<br />
forming resonators of significant quality factors that may e.g. be used<br />
in novel filtering devices for optical telecommunications (1330 and 1550<br />
nm). We show what influence parameters like etching depth and vertical<br />
contrast have on attainable quality factors and on transmission as well<br />
as coupling efficiencies. First results are presented on the use of ultra low<br />
index substrates.<br />
HL 20.4 Di 16:00 H17<br />
Emitting quantum dots under photonic confinement: composite<br />
materials design and fabrication — •Nikolai Gaponik 1 , Richard<br />
Capek 1 , Alexander Eychmüller 1 , Andrey Rogach 2 , Clivia Sotomayor<br />
Torres 3 , and Sergei Romanov 3 — 1 Institute of Physical<br />
Chemistry, University of Hamburg, 20146 Hamburg — 2 Photonics and<br />
Optoelectronics Group, Department of Physics and CeNS, University<br />
of Munich, 80799 Munich — 3 Institute of Materials Science and Department<br />
of Electrical and Information Engineering, University of Wuppertal,<br />
42097 Wuppertal<br />
Strongly luminescent colloidal quantum dots (QDs) were integrated<br />
into various types of opal-based photonic structures and microcavities.<br />
The post-preparative treatment of QD surface was demonstrated to be a<br />
powerful tool to give precise control over the luminescent photonic composite<br />
materials properties. Both the layer-by-layer assembly and solventcontrolled<br />
precipitation techniques were optimized to be used for formation<br />
and selective modification of light-emitting hetero-opals. Structural<br />
and optical properties of fabricated composite materials are reported.<br />
HL 20.5 Di 16:15 H17<br />
Cavity QED phenomena in Photonic Crystal Microcavities containing<br />
self-assembled Quantum Dots — •A. F. Kreß, F. Hofbauer,<br />
H. J. Krenner, D. Schuh, R. Meyer, and J. J. Finley —<br />
Walter Schottky Institut, TU München, 85748 Garching, Germany<br />
We present optical investigations of active photonic crystal defect mircocavities<br />
(PCµC) formed from a hexagonal lattice of air-holes in a GaAs-<br />
(Al)GaAs slab waveguide. Incorporation of one or more layers of self assembled<br />
InGaAs quantum dots (QD) into the waveguide enable us to<br />
directly probe the nature of the cavity modes using spatially resolved<br />
photoluminescence (µPL) spectroscopy. Moreover, cavity-QED phenomena<br />
have been directly observed using time resolved spectroscopy.<br />
The fully localised PCµC modes show strongly enhanced light emission<br />
with Q>500 for a modevolume of ∼ 3(λ/n) 3 . Time resolved measurements<br />
clearly demonstrate Purcell enhancement of the spontaneous<br />
emission rate with Purcell factors up to ∼4 having been observed.<br />
Control of the design and symmetry of the PCµC allows us to engineer<br />
the cavity modes. µPL measurements on a series of H2 PCµCs<br />
demonstrate our ability to tune the wavelength of the cavity modes over<br />
∼ ±30nm around ∼950nm with a precision better than ∼1nm. Tuneable<br />
cavity states are investigated in different hexagonal crystals and exhibit<br />
mode structure in good accordance with our calculations. Improved<br />
PCµC designs for reduced symmetry ultra high Q-cavities will also be<br />
presented. Finally, we will discuss a device concept for an electronically<br />
tuneable PCµC for planned single QD cavity QED experiments.<br />
HL 20.6 Di 16:30 H17<br />
Metal-Dielectric Photonic Crystals from Gold Coated opals<br />
— •Andrei Susha 1 , Paul Miclea 2 , Clivia Sotomayor Torres 2 ,<br />
Sergei Romanov 2 , and Frank Caruso 3 — 1 Dept. of Physics, University<br />
of Munich, 80799, Germany — 2 Inst. of Materials Science, Dept. of<br />
Electrical and Information Engineering, University of Wuppertal, 42097,<br />
Germany — 3 Dept. of Chemical and Biomolecular Engineering, University<br />
of Melbourne, Victoria 3010, Australia<br />
The promise of metal-dielectric (MD) opals is to be photonic crystals<br />
(PhC) with wide and robust photonic bandgap (PBG). To prepare<br />
films of MD opals, the latex spheres were coated by 5nm Au nanoparticles<br />
(NP). The angular-resolved reflectance spectroscopy in the visible<br />
and near-infrared ranges, the surface diffraction and light scattering were<br />
used to study their PBG.<br />
The surface plasmon resonance of Au NPs changes in opals from the<br />
single peak to the set of peaks in correspondence to the shape of NCs<br />
aggregates. The diffraction resonance in Au-opals evolves away from the<br />
dielectric-type behaviour, when it overlaps the plasmon resonance. Increase<br />
of the Au content up to 50 wt. emerging bands with unusual<br />
angular dispersion. Experimental data are discussed in the light of theory<br />
predictions.