Crystalline
Defects in Silicon
Like
anything else in this world, crystals inherently possess imperfections,
or what we often refer to as
'crystalline defects'.
The presence of most of these crystalline defects is undesirable in
silicon wafers, although certain types of 'defects' are essential in
semiconductor manufacturing. Engineers in the semiconductor industry
must be aware of, if not knowledgeable on, the various types of silicon
crystal defects, since these defects can affect various aspects of
semiconductor manufacturing - from production yields to product
reliability.
Crystalline defects may be
classified into four categories according to their geometry.
These categories are: 1) zero-dimensional or
'point' defects;
2) one-dimensional or
'line' defects;
3) two-dimensional or
'area' defects;
and 4) three-dimensional or
'volume' defects.
Table 1 presents the commonly-encountered defects under each of these
categories.
Table 1.
Examples of Crystalline Defects
|
Defect Type |
Examples |
|
Point or
Zero-Dimensional Defects |
Vacancy Defects
Interstitial Defects
Frenkel Defects
Extrinsic Defects |
|
Line or
One-Dimensional Defects |
Straight Dislocations
(edge or screw)
Dislocation Loops |
|
Area or
Two-Dimensional Defects |
Stacking Faults
Twins
Grain Boundaries |
|
Volume or
Three-Dimensional Defects |
Precipitates
Voids |
There are
many forms of crystal
point defects. A defect wherein a silicon atom is missing from one of
these sites is known as a
'vacancy'
defect. If an atom is
located in a non-lattice site within the crystal, then it is said to be
an 'interstitial'
defect. If the
interstitial defect involves a silicon atom at an interstitial site
within a silicon crystal, then it is referred to as a
'self-interstitial'
defect. Vacancies and
self-interstitial defects are classified as
intrinsic point defects.
If an atom leaves its site
in the lattice (thereby creating a vacancy) and then moves to the
surface of the crystal, then it becomes a
'Schottky'
defect. On the other hand, an atom that vacates its position in
the lattice and transfers to an interstitial position in the crystal is
known as a
'Frenkel'
defect. The formation of a Frenkel defect therefore produces two defects
within the lattice - a vacancy and the interstitial defect, while the
formation of a Schottky defect leaves only one defect within the
lattice, i.e., a vacancy. Aside from the formation of Schottky and
Frenkel defects, there's a third mechanism by which an intrinsic point
defect may be formed, i.e., the movement of a surface atom into an
interstitial site.
Extrinsic
point defects,
which are point defects involving foreign atoms, are even more critical
than intrinsic point defects. When a non-silicon atom moves into a
lattice site normally occupied by a silicon atom, then it becomes a
'substitutional
impurity.'
If a non-silicon atom occupies a non-lattice site, then it is referred
to as an
'interstitial
impurity.'
Foreign atoms
involved in the formation of extrinsic defects usually come from dopants,
oxygen, carbon, and metals.
The presence
of point defects is important in the kinetics of diffusion and
oxidation. The rate at which diffusion of dopants occurs is
dependent on the concentration of vacancies. This is also true for
oxidation of silicon.
<Proceed to Page 2 -
Dislocations>
<Proceed to Page 3 - Area and
Volume Defects>
See Also:
Crystal Defect Effects;
Incoming
Wafers;
Epitaxy;
Polysilicon;
Ion
Implant; Gettering;
Crystal
Growing
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