Erasmus Langer
Siegfried Selberherr
Bindu Balakrishna
Oskar Baumgartner
Hajdin Ceric
Johann Cervenka
Otmar Ertl
Wolfgang Gös
Klaus-Tibor Grasser
Philipp Hehenberger
René Heinzl
Hans Kosina
Goran Milovanovic
Neophytos Neophytou
Roberto Orio
Vassil Palankovski
Mahdi Pourfath
Karl Rupp
Franz Schanovsky
Philipp Schwaha
Ivan Starkov
Franz Stimpfl
Viktor Sverdlov
Oliver Triebl
Stanislav Tyaginov
Martin-Thomas Vasicek
Stanislav Vitanov
Paul-Jürgen Wagner
Thomas Windbacher

Ivan Starkov
MSc
starkov(!at)iue.tuwien.ac.at
Biography:
Ivan Starkov was born in Leningrad in 1983. He studied physics at the State University of St.Petersburg, Russia, where he received the MSc degree in physics in 2007 (his work is devoted to the field of the point source in the two-layered periodic structures). He joined the Institute for Microelectronics in January 2009, where he is currently working on his doctoral degree. His scientific interests include hot-carrier reliability issues, Monte-Carlo simulations, device modeling in general as well as the Green's function formalism in the condensed matter physics.

The Modeling of Hot Carrier Reliability

As the linear dimensions of a MOSFET are reduced to the sub-0.1μm range, the Bias Temperature Instability (BTI), Hot-Carrier Injection (HCI) and the Time-dependent Dielectric Breakdown (TDDB) become very crucial reliability concerns. Due to the drastic increase of the electric field in the channel of modern MOSFETs, carriers are heated and then gain sufficient energy to produce damage in an insulator film. From a microscopic point of view, BTI and HCI are closely linked, however it has been repeatedly reported in the literature that HCI-induced degradation has a larger permanent component. This circumstance suggests that another additional (with respect to BTI) mechanism contributes to the HCI-related damage. One may conditionally separate the hot carrier reliability modeling into two main sections. The first is related to the energetics of the Si-O, Si-H and Si-Si bond-breakage, while the second is devoted to the calculation of the non-equilibrium distribution function of the carriers in the channel. Because of the great impact contributed by the heated particles to the degradation process, the high-energetical tails of the energy distribution should be carefully modeled. In this connection the full-band device Monte-Carlo method is very well suited. Such an approach allows us not only to model the distribution function but also to calculate such relevant parameters as the carrier dynamic temperature, velocity, electrical field distribution, etc. for real (i.e. industrial) MOSFETs.


Distribution function of hot electrons in the channel of a MOSFET calculated using the Monte-Carlo full-band method for the source-drain voltage of 50V. The coordinate varies along the channel and high-energetical tails of the distribution function are pronounced.


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