09.12.2012 Views

Plenarvorträge - DPG-Tagungen

Plenarvorträge - DPG-Tagungen

Plenarvorträge - DPG-Tagungen

SHOW MORE
SHOW LESS

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.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!