Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
Halbleiterphysik Montag<br />
concentration, which was confirmed by SIMS measurements, neither segregation<br />
nor coulombic repulsion plays an important role in the system<br />
HL 10 Baulemente<br />
discussed here.<br />
This work was supported by the DFG, SFB 602 TP A7.<br />
Zeit: Montag 15:15–16:30 Raum: H13<br />
HL 10.1 Mo 15:15 H13<br />
Efficiency of High-Brightness AlGaInP LEDs: Model and Experiment<br />
— •P. Altieri, A. Jaeger, R. Windisch, N. Linder, P.<br />
Stauss, R. Oberschmid, and K. Streubel — OSRAM Opto Semiconductors<br />
GmbH, Wernerwerkstr. 2, 93049 Regensburg<br />
We present a quantitative analysis of the internal quantum efficiency<br />
of high-brightness AlGaInP light-emitting devices (LEDs) with an emission<br />
wavelength ranging from 650 nm to 560 nm. The wavelength is<br />
adjusted by varying the Aluminum content in the active region. The<br />
evaluation is based on measurements of the external quantum efficiency<br />
of the LEDs as a function of the operating current (0.1-20 mA) and<br />
temperature (298-360 K). The determination of the internal quantum efficiency<br />
is performed by means of a model that takes into account the<br />
radiative and nonradiative recombination in the active layer, the diffusive<br />
leakage of charge carriers into the confining InAlP layers and the influence<br />
of photon recycling on the light extraction efficiency. In the current<br />
range here analyzed red emitting LEDs show maximum internal quantum<br />
efficiencies close to 100 %. The maximum efficiency decreases with<br />
decreasing wavelength down to about 7 % for green LEDs. This reduction<br />
is mainly due to leakage which accounts for the loss of about 75 % of the<br />
injected carriers. In addition, the nonradiative recombination increases<br />
by approximately one order of magnitude from red to green LEDs.<br />
HL 10.2 Mo 15:30 H13<br />
The Source-Gated Thin-Film Transistor — •Thomas Lindner 1 ,<br />
Gernot Paasch 1 , and Susanne Scheinert 2 — 1 IFW Dresden —<br />
2 TU Ilmenau<br />
In thin-film transistors as usual the channel is controlled by the gate<br />
and the current saturates when the drain end of the channel becomes<br />
depleted due to the drain voltage. For this operation the channel contacts<br />
to source and drain must be ohmic. Recently, source-gated thin-film<br />
transistors (SGT) made by undoped a-Si:H have been introduced 1 . In the<br />
SGT there is no direct contact between source and the channel. This design<br />
is essentially the same as that one of the top contact (TOC) organic<br />
field-effect transistor (FET) 2,3 . In the SGT in addition the source contact<br />
is chosen as a depletion (Schottky) contact. In Refs.(2,3) the TOC<br />
FET has been investigated also for Schottky contacts. In contrast to the<br />
advantages of the SGT proposed in Ref.(1) we found that apart from<br />
the unusual voltage dependencies of the current, the main feature of the<br />
Schottky-contacted TOC FET is a strongly reduced current due to the<br />
series resistance between source and the channel. Here a detailed simulation<br />
study for the a-Si:H based SGT is presented revealing the operation<br />
mode of this device.<br />
1 J.M. Shannon, E.G. Gerstner, IEEE ED Letters 24 (2003) 405.<br />
2 S. Scheinert, G. Paasch, T. Lindner, Synth. Met. 137 (2003) 1451.<br />
3 T. Lindner, G. Paasch, S. Scheinert, J. Mat. Res., submitted.<br />
HL 10.3 Mo 15:45 H13<br />
Patterning of sub 50 nm structures for diffusion investigations<br />
in vertical Double-Gate MOSFETs — •Jürgen Moers 1 , Stefan<br />
Trellenkamp 1 , Susan Kluth 2 , Patrick Kluth 2 , David Alvarez<br />
3,4 , Johannes Kretz 4 , Siegfried Mantl 1 , and Hans Lüth 1<br />
— 1 Institute of Thin Films and Interfaces, Forschungszentrum Jülich, D-<br />
52425 Jülich — 2 Australien National University, Canberra, ACT 0200,<br />
Australia — 3 IMEC, Kapeldreef 75, B-3001 Leuven, Belgium — 4 Infineon<br />
Technologies AG, D-81730 Munich<br />
The tremendous increase in computational efficiency was made possible<br />
by shrinking the dimension of microelectronic devices. This downsizing<br />
led to the well known Short Channel Effects (SCE). To account for these<br />
SCE the lateral layout was improved. For future CMOS applications this<br />
will be not sufficient, therefore new architectures must be investigated.<br />
One architecture is the Double-Gate-MOSFET, where the channel forming<br />
thin silicon layer is sandwiched between two gates; these two gates<br />
control the electric field in the silicon very efficiently and hence reduce<br />
SCE. Heart of this device is a silicon ridge of ∼20 nm width, in which<br />
the dopants are implanted. The channel length of the device is defined<br />
by the implantation energy and the diffusion during the subsequent thermal<br />
treatment. Therefore it is essential to investigate the diffusion in<br />
nanostructures.<br />
Sub 50 nm structures in silicon were prepared using electron beam<br />
lithography and high selective reactive ion etching. First results show a<br />
different boron diffusion due to reduced transient enhanced diffusion. A<br />
qualitative interpretation of the effects are given.<br />
HL 10.4 Mo 16:00 H13<br />
Electrical characterization of temporary devices fabricated<br />
with a double-tip AFM on semiconductive surfaces — •A.-D.<br />
Müller 1 , F. Müller 1 , T.D. Long 1 , L.Q.T. Dung 1 , J. Mehner 2 ,<br />
and M. Hietschold 1 — 1 Chemnitz University of Technology, Institute<br />
of Physics, Solid Surface Analysis Group, 09107 Chemnitz — 2 Chemnitz<br />
University of Technology, Institute of Electrical Engineering and<br />
Information Technology, 09107 Chemnitz<br />
Using a multiple cantilever device, semiconductor devices can be created<br />
temporarily on a semiconductor`s surface to perform an electrical<br />
measurement. The obtained electrical characteristics of such devices represent<br />
the local electrical surface properties at the moment of the measurement.<br />
This contribution presents the application of a double cantilever, which<br />
has two tips with a lateral distance of 10 µm. Each tip has its own vertical<br />
actuator, so that they can be placed on the surface independently of<br />
each other with a detectable contact force in an Atomic Force Microscope<br />
set-up. The observed electrical characteristics are compared with circuit<br />
simulations using a MESFET model instead of the temporary device. On<br />
silicon (111) with a natural oxide layer, for instance, a high surface conductivity<br />
and a high barrier at the temporarily formed Pt/Si-interfaces<br />
have been found.<br />
HL 10.5 Mo 16:15 H13<br />
Simulation and fabrication of complementary tunneling transistors<br />
in silicon — •Peng-Fei Wang, Thomas Nirschl, Marcus<br />
Weis, Doris Schmitt-Landsiedel, and Walter Hansch — Institute<br />
for Technical Electronics, Technical University Munich, Arcisstr. 21,<br />
80333 Munich, Germany<br />
In this paper, a surface-tunneling transistor called TFET is fabricated<br />
using the CMOS compatible technologies. The gate controlled band-toband<br />
tunneling is realized in this transistor. The gate controlled surface<br />
Esaki tunneling current is also observed at room temperature. Due to the<br />
distinct working principle of this novel transistor, the low sub-threshold<br />
leakage current and perfect drain current saturation can be obtained.<br />
Compared to the conventional NMOS, the lower leakage current and<br />
smaller Vth roll-off can be achieved. Since the impact ionization in this<br />
transistor is caused by the electrons injected from tunneling junction,<br />
TFET is also a hot electron transistor where the impact ionization can<br />
be controlled by the gate voltage. In addition, the complementary TEFT<br />
are fabricated on the same silicon substrate. The performances of the<br />
n-channel TFET and the p-channel TFET will be discussed in detail.