hey guys in previous
videos I've talked
about sputtering and my vacuum chamber
in general but in this video I wanted to
spend a little more time talking about
the actual sputtered parameters and a
few more details in case you wanted to
set up a similar system of your own for
this demonstration I'll sputter some
indium tin oxide and as it turned out I
repaired my cracked disk just by gluing
it down to a thin piece of brass so I
put the whole thing down onto the
sputter head and then clamp it down and
then attach the sputter shield on top of
that so the shield is connected to the
same electrical potential as the base of
the chamber all that aluminum and the
center of the sputter head is isolated
from it however when I checked with an
ohm meter I found a couple mega ohms
resistance and I think this is actually
from the cooling water that's
circulating through the sputter head I
put the bell jar on top and as you can
see there's quite a bit of sputter or
overshoot kind of on the inside of the
bell jar there this is how the system is
plumbed so we have the bell jar here the
diffusion pump here with a butterfly
valve here a valve between the diffusion
pump and the mechanical pump and then
another valve between the chamber and
the mechanical pump so right now the
system is idling with basically all the
valves closed and what I want to do is
pump down the chamber so I'm going to
open this valve here and what that's
going to do is allow the all the air
inside the bell jar to be pumped out by
the mechanical pump directly so I'm
looking at the pressure in the chamber
with a thermocouple gauge and we can see
it's coming down slowly the pump down
with with this size chamber and pump
takes about five or ten minutes
eventually the thing will level off at
about 50 Milot or when the mechanical
pump has done all it can do we want to
switch over to the diffusion pump and we
do that by closing this valve and then
opening this valve and opening this
valve and what that will do is allow a
path to go straight from the chamber
through the diffusion pump to the
mechanical pump and eventually venting
out to the atmosphere
the reason we need all these different
valves is because we can't ever let the
diffusion pump come up to atmosphere so
we can't just pull ruff-ruff pump the
chamber down through the diffusion pump
because this all the oil in here would
be exposed to air atmospheric pressure
air which would be a bad news situation
the diffusion pump produces much higher
vacuums than the mechanical pump can and
after a few minutes of being pumped with
both of these pumps in serial the
chamber pressure is down to about 3 or 4
times 10 to the -5 millibar and we're
using a penning gage here to show the
chamber pressure now as you can see the
thermocouple gage that originally showed
the rough vacuum state of the chamber is
no longer useful because it's reading
off scale if we wanted to thermally
evaporate something we would basically
be ready now where the chamber is at a
good vacuum and we could heat something
up and evaporate it as I showed in
another video
however for sputtering we actually need
to reintroduce gas molecules to the
chamber so we can use those gas
molecules to perform the sputtering in
this case we're going to be using argon
I wanted to have a better handle on
exactly what was going on with the gas
flows in this system and also wanted the
ability to do a process called reactive
sputtering later so I bought a couple of
flow meters and I'm going to show you
how to calculate the chamber pressure
based on the flow rate in and a known
pumping speed so we measured that the
chamber pressure is about 3 times 10 to
the minus 5 millibar when there's
nothing apparently going into the
chamber and what we're going to do is
open one of these flow meters a bit so
that there is three FCC m in this case
of oxygen going into the chamber so an
SCCM is a standard cubic centimeter per
minute after setting the flow meter to 3
SCCM
we've noticed that the chamber pressure
has risen up to about 5 times 10 to the
minus 4 millibar so here's a simple
equation that will come in quite handy
if you're working with a vacuum chamber
it's pressure equals the gas load
by the pumping speed and in this case we
know what the gas load is because we're
introducing it through that flow meter
and we know what the pressure is because
we just measured it but it would be nice
to know what the pumping speed is so
that we can use that in future equations
and to figure out things in the future
so we have to do some conversions here
the gas load is three SCCM minus zero
zero because it was we weren't
intentionally adding anything to the
chamber and then we have to convert
standard cubic centimeters per minute to
millibar liters per second and I'll talk
about those units in a sec so that's
what this is for
and then there's a correction factor for
the flow meter so you'll notice that the
flow meter looks sort of backwards from
the how they're often set up with the
valve on the top this time and the trick
is that when you're using a flow meter
for vacuum applications you want that
that needle valve to be on the output so
that the valve body itself that the flow
meter tube itself is actually
pressurized it doesn't work to do it the
other way because in a high vacuum
situation the gas is in molecular flow
it's not in viscous flow and there's
really nothing to push that flow meter
ball up in a normal pattern and so it
just Bob's around it's practically
unusable so anyway this correction
factor takes into account that the flow
meter body is not at ambient pressure
it's actually at about five psi and five
psi is what's coming out of my welding
cylinders and going into the flow meter
so the fact that there's pressure in
there means that the gas is a little
more dense that it normally would be at
standard conditions and the correction
factor conveniently is just the square
root of the absolute pressure ratio so
we've got basically 14.7 PSI is ambient
and it's 20 absolute going in which is
five psi gauge the pressure is just the
difference of the two readings that we
took with the pen engage and when we do
all the math this comes out to 125
liters per second which if we check the
diffusion pump manual for online it's
actually very close to the real value
surprise
clothes in fact so about this pumping
speed the unit leader per second is
sometimes a little misleading I think
the best way to think about this is just
imagine that you had in your hands a
container that's one liter big and 125
liters per second means that you just
put that container into the vacuum
chamber and then close it and remove it
from the vacuum chamber and empty it out
and then do that again 125 times per
second you'd have 125 liters per second
pumping speed so if the chamber were
completely empty and had no molecules in
there whatsoever then you wouldn't
actually be moving any atoms at all so
the pumping speed doesn't really
describe how much mass you're actually
removing from the chamber it only
describes the potential to remove mass
from the chamber if we look at a graph
of a diffusion pumps pumping speed
versus pressure we notice that it's
completely constant all the way down to
essentially zero and at first this seems
really great you'd think oh man this
pump will you know get down to deep
space vacuum I mean it's pumping the
speed is constant all the way to zero
but as I described that's only the
volume once the chamber pressure gets
low enough moving that volume out isn't
really all that helpful so what you can
do is just get a bigger and bigger pump
so the bigger and bigger container being
placed into the vacuum chamber and
closed and removed you'll keep removing
more molecules you can just never really
get all the way to zero a lot of
academic papers and white papers
describe sputtering process where they
make a big deal out of the flow rate
going into the chamber and I always
wondered why they seemed to care more
about the flow rate than the pressure I
mean it seems like if you're you know
interested in this sputtering process
and you know what the argon pressure is
it doesn't really matter what the flow
rate should be because really the
physics of this problem only depend on
pressure and that's true but there's a
big catch the trick is that you want to
have a lot of argon as much as possible
basically flowing into your chamber to
wash away all of the byproducts and
outgassing things you know trace
elements and things that you don't want
part of the process so ideally we would
want the chamber completely
empty and then we put argon in so that
the only thing in there is argon and we
can control the process very carefully
in reality there will be a lot of water
vapor and carbon monoxide and decomposed
bits of the substrate and all kinds of
things floating around in the chamber so
what we want is a high pumping speed and
also a high argon flow rate to make sure
that the gas is fresh in the chamber the
problem is that the pressure also needs
to be pretty low to prevent a
contamination and to prevent these trace
gases from being incorporated into the
substrate coating so we kind of want
everything all at once we want you know
a lot of pumping and a lot of fresh gas
and all this stuff and we compromised
and the main point that you know causes
the compromise to be made is the size of
the pump so 125 litres per second is not
very big as far as industry is concerned
most industrial setups would have like a
turbo molecular pump running 2 or 3 or
even 500 liters per second so I'm going
to scale down most of the values that
I'm going to do in my chamber by about a
factor of 3 to 5 to compensate for this
for sputtering this Itoi found that
fairly low pressures of pure argon can
actually produce fairly good coatings
despite what most of the literature says
I found one paper that talked about long
throw sputtering with just pure argon so
to set up I'm going to set the argon
flow meter to 6 to 8 SC cm and no oxygen
at all and there's another compensation
factor to worry about since this flow
meter is passing are gone and it was
calibrated for air we get to multiply it
by 1.2 in addition to the pressure
compensation factor argon is more dense
than air and so it can push that little
ball up more easily so we have to
compensate for that
after getting the flow rate dialed and I
turn on the RF power source
and turn it up to just about 10 or 20
watts at this point there is no plasma
in the chamber because the pressure is
too low and the reflected power is
fairly high because there's no plasma to
take up that energy
to get the plasma started I close the
valve leading to the diffusion pump just
momentarily any pressure will come up
high enough for the plasma to be ignited
as soon as the ignites I open the
diffusion pump valve because once the
plasma is there it can be sustained at a
much lower pressure I turn the power up
to about 40 watts and after just about
30 seconds of stabilization we can see
that the sensor head is picking up
deposited IT oh it's not a particularly
fast process so we're only getting a few
tenths of an angstrom per second which
means that we need to spend about 30 to
60 minutes on this to get a usable i teo
coating it is possible to turn up the
power and just make the process go
faster but then that also changes how
this thing works and so there's a lot of
variables in play that I myself don't
fully understand after reading a bunch
of academic papers it's pretty clear
that there's quite a bit of contention
even in industrial and research settings
just a few of the important factors of
the distance from the sputter target to
the substrate the RF power being put
into it the geometry of the sputter head
the substrate temperature the target
temperature DC bias applied to either
the substrate or the target argon flow
rate oxygen flow rate total pressure of
the system I mean it just goes on and on
and so dialing in all of these variables
is difficult and I think there's also
multiple solutions that will work well
enough for consumer electronic type
devices which is why there's so many
different kinds of process described in
the academic papers this slide has about
200 nanometers of IPO deposited in just
the way that I showed in this video and
I'm pretty happy with this this is
coming in at about a hundred ohms across
the slide like that which is more than
an order of magnitude improvement over
my last batch so I think with just a
little more tweaking I'll get down to
the I guess industry standard of maybe
20 ohms per square if not it's not
really that big of a deal for making
things like LCDs and displays like that
the surface resistivity of the coating
is not terribly important okay well I
hope that was helpful let me know if you
have any questions about building your
own sputtered system you definitely
don't have to take it to the extreme
that I did for non magnetron sputtering
you don't really need half the equipment
here you can really do it with just a
jar vacuum pump and an a high voltage
supply so I was thinking about making a
video just showing it sort of a cut-down
version to do it with minimal stuff let
me know if you'd have interested in
seeing that okay see you next time bye earn money online by clicking, online money income site, money earning sites, online earning sites, best website to earn money, free money earning sites, money earning websites, get money online, online earning tips, online earning without investment, earn money online without investment for students, earn money by clicking ads, earn money online without investment, online earn money website, online jobs to earn money, best online income site, top 10 online money earning sites, easy income online, easy online earning, earn money online from home, make money online legit, earn money online free fast and easy,
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