Erasmus Langer
Siegfried Selberherr
 
Elaf Al-Ani
Tesfaye Ayalew
Hajdin Ceric
Martin Della-Mea 
Siddhartha Dhar
Robert Entner 
Andreas Gehring 
Klaus-Tibor Grasser 
René Heinzl 
Clemens Heitzinger
Christian Hollauer
Stefan Holzer
Andreas Hössinger 
Gerhard Karlowatz 
Robert Kosik 
Hans Kosina 
Alexandre Nentchev
Vassil Palankovski
Mahdi Pourfath 
Philipp Schwaha
Alireza Sheikoleslami 
Viktor Sverdlov 
Stephan Enzo Ungersböck 
Stephan Wagner 
Wilfried Wessner
Robert Wittmann 

 

   
 

Stephan Enzo Ungersböck
Dipl.-Ing.
ungersboeck(!at)iue.tuwien.ac.at
Biography:
Stephan Enzo Ungersböck was born in Vienna, Austria, in 1977. He studied physics at the Technische Universität Wien, where he received the degree of Diplomingenieur in May 2002. He joined the Institute for Microelectronics in June 2002, where he is currently working on his doctoral degree. He held a visiting research position at the Samsung Advanced Institute of Technology in Seoul, South Korea, in summer 2003. His scientific interests include Monte Carlo simulation, band structure calculations, simulation of carbon nanotubes, and quantum mechanical confinement in submicron MOSFETs.

Self-Consistent Simulation of Universal Mobility in Strained Si MOSFETs

Strain in silicon is able to enhance the effective mobility of both n-channel and p-channel MOSFETs by around 70% and 100%, respectively. In SOI and DG MOSFETs the thickness of the Si substrate has a major impact on the device performance. Accurate models for the mobility of DG-, SOI-, or strained Si/SiGe MOSFETs require a simulation of the inversion layer mobility. The strong confinement leads to the quantization of the electron (hole) state normal to the interface and the conduction (valence) bands split into a system of discrete subbands. In the direction parallel to the interface the charge carriers behave like free particles. This system is called 2D electron gas and exhibits different scattering rates than the bulk case and additional scattering mechanisms caused by surface roughness and oxide charges. The scattering mechanisms have been introduced in an MC simulator suited for the simulation of the inversion layer mobility. In order to extract the universal mobility curves, the MC simulator has been coupled to a Schrödinger-Poisson solver.

The full-band structure is an indispensable ingredient of hot-electron and hole transport in general. The MC simulator VMC, which is based on the approximation of non-parabolic bands, is being extended to allow full-band MC simulations. A band structure simulation tool based on the non-local empirical pseudopotential method with relativistic corrections was extended to extract the band structure of strained silicon layers grown on silicon-germanium substrates. This will allow the simulation of novel devices including strain effects in two and three dimensions.


The performance of Schottky barrier carbon nanotube field effect transistors (CNTFETs) depends critically on the device geometry. Asymmetric gate contacts, the drain- and source contact thickness, and non-homogeneous dielectrics above and below the nanotube influence the device operation. CNTFETs were optimized with respect to the subthreshold slope, high on-off ratio, and large on-currents. It was shown that the use of a thin needle-like source contact is favorable, whereas large drain contacts can decrease the off-current. The best performance improvements can be achieved using asymmetric gates centered above the source contact, where the position and length of the gate contact varies with the oxide thickness and high-k materials on top of the CNT and low-k materials below the tube. It was demonstrated that by optimization of the geometry the subthreshold slope can be reduced by a factor of two, reaching a value of 100 mV/dec for devices with oxide thicknesses of 5 nm.


Self-consistent simulation result
of universal mobility curve and
comparison to experimental results.
   
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