Materials Science
Transport properties of bulk semiconductors are strongly influenced
by intrinsic and extrinsic defects. Introduction of extrinsic defects
via p- and n-type doping is crucial to building semiconductor
devices. An example of p-type doping is boron-implanted silicon.
Here, boron ions impinge on and penetrate a silicon sample. The doping
profile, that is, the concentration distribution of the boron ions
as a function of implantation depth, should be as sharp as possible
since sharp profiles allow the fabrication of small devices and fast
computers.
Since ion implantation breaks bonds in the silicon sample, these broken
bonds have to be ``repaired'' since they act as carrier traps otherwise.
A standard way to repair the damage done, is to anneal
the sample. A major problem that arises upon annealing, is that boron
diffuses at least 100 times faster in boron-implanted silicon than in
bulk silicon. This fast initial diffusion -- the so-called transient
enhanced diffusion -- leads to broad doping profiles and limits the
size reduction that can be obtained in submicron Si-based devices.
Interstitial and extended {311} defects in silicon are believed to
be the reason for the transient enhanced diffusion in silicon. Our
work is an ab-initio description of di-interstitial defects,
that for the first time identifies the structure of the characteristic
P6 di-interstitial defect. In the medium and long-term, we will
understand formation mechanisms of extended defects in Si and their
interaction with other impurities such as boron or carbon.
To cite this page:
Defects in Silicon
<http://www.physics.ohio-state.edu/~aulbur/sidefect/sidefect.html>