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 

 

   
 

Gerhard Karlowatz
Dipl.-Ing.
karlowatz(!at)iue.tuwien.ac.at
Biography:
Gerhard Karlowatz was born in Mödling, Austria, in 1972. He studied physics at the Technische Universität Wien, where he received the degree of Diplomingenieur in October 2003. He joined the Institute for Microelectronics in December 2003, where he is currently working on his doctoral degree. His scientific interests include Monte Carlo methods and organic devices.

Full-Band Monte Carlo Device Simulation

The success of TCAD depends on the reliability and efficency of the computer models used. Due to the rapid progress of Si technology and the introduction of new device types and materials, known models are continously being improved and new models are being developed. During this development process it is important to compare the results of TCAD simulations to those obtained by more fundamental methods.
Here the Monte Carlo (MC) approach, in which the movement of electrons or holes within a material of interest is sampled over a simulation time period, proves to be very successful. As computational power increases, MC methods can even be used in combination with TCAD device simulations, helping to solve hot carrier and short channel problems.

Basically there are two representations of the band structure of a material in an MC simulator: namely analytical expressions, as the parabolic or non-parabolic approximations, or a full band structure. In the latter case the band structure is calculated for a representable part of the first Brillouin zone and then passed to the MC simulator in form of a three-dimensional mesh. Despite the higher computational costs, it is necessary to use the full-band approach for hot carrier problems, because an accurate representation of the band structure at higher energies is essential here.
It has been shown that these computational costs can be kept sufficiently low when using tetrahedrons as elementary mesh elements and isotropic scattering models which only depend on the density-of-states (DOS). Since the density of states is given by an integral over an equi-energy surface in the Brillouin zone, and this surface is a plane area within a tetrahedron, fast calculation of the DOS and fast determination of the carrier state after a scattering process are obtained. Currently the expansion of the Vienna Monte Carlo Simulator (VMC) to a full-band simulator is in progress, with the further goal to integrate this simulator with Minimos-NT, which then will provide the feature of two- or three-dimensionsional combined TCAD/MC device simulations.


Contribution of the first four conduction-bands
to the density of states (DOS) of silicon
   
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