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The abbreviation "LOCOS" stands for "Local Oxidation of Silicon"
and was almost a synonym for MOS devices, or more precisely, for the
insulation between single transistors. LOCOS makes the isolation between
MOS transistors considerably easier then between bipolar transistors,
cf. the drawings discussed before: |
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For
bipolar
transistors, you have to separate the collectors. This involves an
epitaxial layer and some deep diffusion around every transistor. |
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For
MOS
transistors, no isolation would be needed weren't it for the possible
parasitic transistors. And this problem can be solved by making the "gate
oxide" of the parasitic transistors - which then is called
field oxide - sufficiently thick. |
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The thick field oxide has been made
by the LOCOS process from the beginning of MOS technology until
presently, when LOCOS was supplanted by the "box isolation technique", also known as
"STI" for "Shallow trench isolation".
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Since the LOCOS technique is still used,
and gives a good example of how processes are first conceived, are optimized
with every generation, become very complex, and are finally supplanted with
something different, we will treat it here in some detail |
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As the name implies, the goal is to
oxidize Si only locally, wherever a
field oxide is needed. This is necessary for the following reason: |
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Local
(thermal) oxide penetrates into the Si (oxidation is using up
Si!), so the Si - SiO2 interface is lower than the source - drain regions to be made
later. This could not be achieved with oxidizing all of the Si and then
etching off unwanted oxide. |
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For device performance reasons, this is highly
beneficial, if not absolutely necessary. |
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For a local oxidation, the areas of the Si that are
not to be oxidized must be protected by some material that does not allow oxygen diffusion at the
typical oxidation temperatures of (1000 - 1100) 0C. We are
talking electronic materials again! |
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The only material that is "easily" usable is
Silicon nitride,
Si3 N4. It can be
deposited and structured without too much problems and it is compatible with
Si. |
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However, Si3 N4
introduces a major new problem of its own, which can only be solved by making
the process more complicated by involving yet another materials. This gives a
succinct example of the
statement made
before: That materials and processes have to be seen as a unit. |
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Lets see what would happen with just a
Si3 N4 layer protecting parts of the Si
from thermal oxidation. |
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Oxygen diffusion through the oxide already formed
would also oxidize the Si under the Si3 N4; i.e.
there would be some amount of lateral oxidation. Since a given volume of
Si expands by almost a factor of 2 upon oxidation (in other
words: Oxidizing 1cm3 of Si produces almost 2
cm3 of SiO2), the nitride mask is pressed
upwards at the edges as illustrated. |
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With increasing oxidation time and oxide
thickness, pressure under the nitride mask increases, and at some point the
critical yield strength of Si at the
oxidation temperature is exceed. Plastic
deformation will start and dislocations are generated and move into
the Si. Below the edges of the local oxide is now a high density of
dislocations which kill the device and render the Si useless - throw it
out. |
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This is not "theory", but eminently
practical as shown in the TEM picture from the early
days of integrated circuit technology: |
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We are looking through a piece of Si. The
dark lines are the projections of single dislocations, the "dislocations
tangles" corresponds to oxide edges; "E" shows contact
areas (emitters) to the Si.
Another picture can be
found in the link. |
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Actually, it doesn't even need
the oxidation to produce dislocations. Si3 N4
layers are always under large stresses at room temperature and would exert
great shear stresses on the Si; something that can not be tolerated as
soon as the nitride films are more than a few nm thick. |
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We arrive at a simple rule: You
cannot use Si3
N4 directly on Si - never ever. What are we to do
now, to save the concept of local oxidation? |
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We need something between the Si3 N4 mask
and the Si; a thin layer of a material that is compatible with the other
two and that can relieve the stress
building up during oxidation. Something like the oil in you motor, a kind of
grease. |
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This "grease" material is
SiO2, as you might have guessed - it was already
mentioned before under its proper
name of "buffer oxide". The hard
Si3 N4 (which is a ceramic that is very hard not
yielding at a "low" temperature of just about 1000
oC), is now pressing down on something "soft", and the
stress felt by the Si will not reach the yield stress - if everything is
done right. |
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The situation now looks like this |
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No more dislocations, but a comparatively large
lateral oxidation instead, leading to a configuration known as "birds beak" for the obvious reason shown in
the picture to the right (the inserts just are there to help you see the
bird). |
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So we got rid of one problem, but now
we have another one: The lateral extension of the field oxide via the birds
beak is comparable to its thickness and limits the
minimum feature size. |
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While this was not a serious problems in the
early days of IC technology, it could not be tolerated anymore around
the middle of the eighties. |
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One way out was the use of a poly-Si layer
as a sacrificial layer. It was situated on top of the buffer oxide below the
nitride mask and was structured with the mask. It provided some sacrificial
Si for the "birds beak" and the total dimension of the field
oxide could be reduced somewhat. |
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This
process is shown in
comparison with the standard process in the link. |
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But even this was
not good enough anymore for feature sizes around and below 1 µm.
The LOCOS process eventually became a very complicated process complex
in its own right; for the Siemens 16 Mbit DRAM it consisted of more than
12 process steps including: |
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2 oxidations, 2 poly-Si
deposition, 1 lithography, 4 etchings and 2 cleaning
steps. |
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It was one of the decisive "secrets"
for success, and we can learn a simple truth from this: |
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Before new materials and processes
are introduced, the existing materials and processes are driven to extremes!
And that is not only true for the LOCOS process, but for all other
processes. |
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Still, with feature sizes shrinking ever more,
LOCOS reached the end of its useful life-span in the nineties and had to
be replaced by "Box
isolations", a simple concept in theory, but hellishly difficult in
reality. |
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The idea is clear: Etch a hole (with vertical
sidewalls) in the Si wherever you want an oxide, and simple
"fill" it with oxide next. More about this process can be found in
the link above. |
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© H. Föll (Electronic Materials - Script)