صفحه 1:
In the name of Allah
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۳
۳
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Content :
1-Coating system
Specification @- (C00)
2-Chemical vapor depositio Or eO0)
9-0000
وصتا مره مس
3-Physical vapor deposition
C_@ene Cua Cvaporaiva
Gputtericcy
- Cowpare اد له موسوم
صفحه 4:
عنامت Ket UHY ال ميم
Vacuum Marwal 6
ی( Fixtu re : 2 55-55
Monitoring
‘vaporation Sources)
ubstrate heating
ilow discharge unit
jon Source
05-5
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Rough TC
1
vent
High Vacuurn
Valve
Rough Valve
—
Foreline Valve
Cold Trap
High
Vacuum
Pump
Foreline TC
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Rough TC
High Vacuum»
valve
[DX] Rough vaive
۳ وق
امس
Foreline Valve
Foreline TC
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deposition method
The choice of the deposition method depends on factors such
ras
Type of material used as coating and its purity -1
Layer address speed .¥
Substrate temperature -¥
The strength of the layer and its adhesion to the substrate .F
Fapeiderations 2 ~_ ویب
deposition
__-deposition method
Physical vapor deposition
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Ex :SiO
2
SiHa (gas) + O2 (gas)—> SiOz (solid) +
eo
wea 82 9 se 88 Reaction products
gon S—> 85 مه 3s ©8 —> @® andunreacted
In @@ 22 gas out
2+ © هه — هه
Reactants Products diffuse
diffuse to هه 2 away from
the surface forming Surface % te surtace
| 1 reaction reaction 1
2050۱۳۷07 پر desorption
© Silicon atom
@ Oxygen atom
© Hydrogen atom
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UHVCVD (Ultrahigh
vacuum) ۱
APCVD (Atmospheric
ressure)
LPCVD (low pressure)
PECVD (plasma enhanced)
MOCVD (metal organic)
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1-produces layers with excellent uniformity of thickness
Advantas 5/1 pcvp systems deposit films on both sides .
_3:LPCVD systems deposit at least 25 wafers
ata 7
Pressure sensor
و 3-zone furnace
( Wafers
۱ کت[
<< ——— تبت
* : ١
٠
۱ Gas inlet
Quartz tube
Load door
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Gas هه
“showerhead
under a quartz تا نا
under aqurt2 ut
‘window
Single wafer CVD chamber. Adapted from [1]. Single wafer PECVD system,
window
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مه ماهر لس
where J>J, مج عنام
(Grin gin)
3
Precursors
1-RnM + RnY > MY + n(R-R)
(CH3)3Ga + (CH3)3Sb > GaSb + 3C2 ne
et
Osis inntner
Gass (Comacteg are) Sf
le, 88 (Coming ل
p-Gabs (Acivelaye)
1A Ga, As Grating yer)
2-MY + nRH بت 8 + ۷۱ ۳
(CH3)3Ga + AsH3 GaAs + 3CH4
(C2H5)3In + PH + InP + 3C2 H6
n (CH3)3Al + (1-n)(CH3)3 Ga + AsH3 + Aln Gal-n As
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The thickness of the layer is uniform and (i
.independent of the shape of the substrate
The 2-speed deposition is relatively high (10 to 100
‘nm /s)
al.
Sticking and connecting better than phy:
-methods
This method is very suitable for multi-layered and ۴
.complex layers on the tools in the above designs
.Coating of substrate layers is well done .6
.The process can be controlled at normal pressure .¥
full epithecary epithelium with low impurity without—V¥
«any problems
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1. The need for high temperature for reaction, which has a
negative effect on the substrate and the substrate.
2. The risk of hydrogen explosion
3. Most reactive substances are expensive.
4. Acceptable reactions at low temperatures are low.
5. Due to the corrosive nature of the vapors present in the
deposition process, the substrate is also damaged.
6. Control of uniformity is very difficult.
7. The thermodynamic details are very complicated in this
way.
8. Sub-reaction products may occur in undesirable places
inside the compartment, and the exiting of the product of
reactions is sometimes impossible.
صفحه 15:
لا
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امه ام
سح
alumina coated f
Sa
foil tr
<<
chromium coate|
alumina crucible i
vee Tested Tram,
ey
مب
wire hairpin
wire helix
wire basket
/
alumina crucible with wire basket
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270 degree bent
E- Beam 3 electron beam
Evaporation SYS
magnetic
field
evaporation cones
pyrolytic graphite of material
hearth liner
4-pocket rotary
copper hearth
(OV)
beam forming
cathode aperture
filament
recirculating (-10,000 V)
cooling water ۱
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لاتأعررمع6 أمعاعوم / واطاعن
Standard configurations
6 ér 2%
ae OgO
le-Pocket Multi-Pocket 4 ‘Mult-Pocket 6 Carousel
entered 49۳ 60۳ 360° Pan
3 4 5 okW
Standard Multi Pocket Sources that have 3 ً 0 as
its 5 4 150 100۷
been identified by our customers as the 5: 51 5 5
most popular sources are listed to the right. 8 3 3 7
MDC is has made a commitment with sub- 5 1 دم 0۷
component inventory to offer reduced lead ۳ 7 Ae +15KW.
times for standard multipocket sources. 8 4 و 150
6 1 400ce 15kW
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Electron Beam Gun
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ate and film نج
coe cA
_— 2 عمدت
iputtering Target
How plasma results in deposition
5) Deposited at anode:
some Ar,
some impurities
1) Ar- accelerated to cathode
cathode سر anode
2) Neutral یی 5
target species (AD Al
kicked off; ۳ & ~e
ها عت = هر سا رو
سس en موی
o <A
4). may ionize ee سس
ا ox
ره بح 6) Some physical
resputtering of Al by Ar
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Counter electrode
Gas inlet Vacuum pump
1A gas plasma/ts-struck using an RF power source, causing the gas to become
ionized
2-The ions are a¢celérated towards the surface of the target,
3-Atoms of the source-material to break off from the target in vapor form and
coniiense on all surfaces including the substrate.
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Varieties of sputtering experience
Magnetron sputtering use magnets
7-4۲8 + 54 pe
بست 9
® BF =v,
Tons spiral around B field lines
v= 6 x 10° m/s for electron, 7 < 1 mm for 0.1 T
=
B field enhances time of e- in plasma Fe
= more ionization, greater Ar density. +— &
Yo
6.1920/3.155 Now. 5, 2003
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Reactive sputter deposition: Mix reactive gas with noble gas (Ar or Ne).
analogous to PECVD
Ar +
aN
Also useful for oxides: Si0,, TiO, Cr0....
other nitrides: SIN, FeN,...
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Comparison of deposition methods by cvd and
sputtering
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The accumulated layer in the Sputtering method is more denser and more 4
sadhesivepresulting in greater strength یا
In the Sputtering method, in order to clean the inside of the. of
compartment, unlike the cvd method, there is no need for any additional Sputtering
How plasma results in deposition
بيس اوور Disadvantages of
1) Arr accelerated to cathode Al, some Ar, متسه
و
Crush and increase internal #
cathode 7 anode tension
2) Neutral Ye Impurities #
target species (Al)
نا of bare Local temporary loads on the #
بح | © لهس ®yelkv surface
يد لاع انس عد
90 Chemical reactions with #
رس 44 residual gases
inputs
(eg. 00) 6 Some pysieal lonizing other gases such as
resputering of AL by Ar oxygen
DC Sputtering and Magneto #
method«
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Physical
How do we monitor the process? 4
Reflective optical
Optical:
Transmissive
optical
XL12 Multi Crystal Sensor Head Package Includes:
1H Multi Crystal Sensor Head
© Controller
@ 1" Bolt Feedthrough or 2 3/4 Conflat
30” In-Vacuum Cable
18 12 Complementary Quartz Crystals
11 15 Crystal Carriages
2 Sensor Shields
XL12 Mult Crystal Sensor Head
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Crystalline Thickness
1. The crystal begins to oscillate before the accumulation
of the layer
While the crystal is fluctuating slowly, the target atoms .¥
accumulate on it
Given that a really thin layer of any material produces a quasar equivalent
quasar frequency oscillation, Df can measure the mass and, consequently, the
thickness of the layer
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Optical Thickness
NI
Click to continue
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Extractor ۱ MA D
| ام س٠ Substrate
Ton Source | Ton Beam 5
lon sputtering
Substrate Sputtered Material
7 x
i oN
Ton Source Target
| Jon Beam
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SUBSTRATE HOLDER وى
يبو تك ee
PROBE كتيده
PUMP
GAS
ler ELECTRON
BEAM
EVAPORATOR
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The atomic layer deposition, or Atomic Layer Deposition, which
is briefly called ALD, is one of the advanced methods of
chemical deposition of the material from the vapor phase.
The basis of the atomic atomic layer is the passage of the
chemical precursors from the substrate into a vacuum
compartment such that in each cycle a atomic layer of the
صفحه 36:
E- Beam Deposition
Substrate
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E- Beam Deposition With IAD
Substrate
صفحه 38:
Electron Beam Deposition
Click to see coating
simulation Substrate
oo Bssisted Oepositica
Substrate
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TR
30
0
70
1
50
20
20
40 42 500 550 300 880 1۳ 750 aon a0 0
1/2۷۹
1۳
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سیسات
Noa ایو
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