C5-2(41-Plasma Etching Part 1)
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Transcript of C5-2(41-Plasma Etching Part 1)
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Plasma etchingPlasma etching
K - JISTK - JISTMaterials Science & Engineering
Nanophotonic semiconductor Materials Lab.1
Bibliography
1. B. Chapman, Glow discharge processes, (Wiley, New York, 1980).
- Classical plasma processing of etching and sputtering
2. D. M. Manos and D. L. Flamm, Plasma etching; An introduction,
(Academic, Boston, 1989).
- Most helpful textbook for the researcher majoring the dry etching.
3. M. Sugawara, Plasma etching; Fundamentals and applications,
(Oxford Univ. Press, New York, 1998).
- Mostly dedicated to the high density plasma sources such as ICP and ECR
4. W. N. G. Hitchon, Plasma processes for semiconductor fabrication,
(Cambridge Univ. Press, Cambridge, 1999)
- Theoretical approach to the plasma etching and plasma deposition process
5. R. J. Shul and S. J. Pearton, Handbook of advanced plasma processing techniques,
(Springer, Heidelberg, 2000).
- Helpful textbook for the researcher in the field of compound semiconductor process
6. http://newton.hanyang.ac.kr/plasma/
- Dedicated to the plasma physics for graduate student in physics
http://newton.hanyang.ac.kr/plasma/http://newton.hanyang.ac.kr/plasma/ -
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7. 1. Introduction
K - JISTK - JISTMaterials Science & Engineering
Nanophotonic semiconductor Materials Lab.3
Etch
removal of unwanted area during the fabrication of
semiconductor
Etching is the most important step in the fabrication ofsemiconductor devices along with a lithography technique.
InGaN mesa for LED
etched by ICPInP via-hole etched by RIE GaAs laser-facet etched by ICP
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Advantage of plasma etching
K - JISTK - JISTMaterials Science & Engineering
Nanophotonic semiconductor Materials Lab.5
Etching can be anisotropic
Less consumption of chemicals; cost, environment impact
Clean process (vacuum)Compatible with automation
Precise pattern transfer
Deep silicon etching for sensor application
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Formation of sheath region
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Nanophotonic semiconductor Materials Lab.6
The fast-moving electrons hitthe wall before the ions do andsome stick to the wall.
The wall charges up negativelyand this negative charge pushesother electrons away at thesame time as attracting positiveions.
The field near the wall holds theelectrons away from the walland accelerates the positiveions toward the wall.
High energy ion bombardment
cf) Generally, the voltage drop couldnt be measured. In practice process
engineers usually monitor the dc potential (relative to ground) of the electrode
instead, which is called dc-bias.
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Materials Science & Engineering
Nanophotonic semiconductor Materials Lab.7
Processes in the sheath region
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K - JISTK - JISTMaterials Science & Engineering
Nanophotonic semiconductor Materials Lab.8
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7. 4. Mechanism of plasma etching
K - JISTK - JISTMaterials Science & Engineering
Nanophotonic semiconductor Materials Lab.9
(a) Physical sputtering - purely
physical process by energetic ion
bombardment
(b) Chemical etching - purely chemical
process by forming volatile by-
product through chemical reaction
between substrate and active
radicals in plasma
(c) Accelerated ion-enhanced etching -
chemical etching + physical
etching: removal of volatile product
is accelerated by energetic ion
bombardment(d) Sidewall-protected (inhibitor driven)
ion-enhanced etching deposition
of etch-resistant layer with ion
bombardment isotropic etching
7. 4. 1. Etch mechanism
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7. 4. 2. Sequential steps in etching
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Nanophotonic semiconductor Materials Lab.10
Formation of active etchant byelectron collisions
Transport of active etchant to thewafer surface
Adsorption of etchant to wafer surface Reaction of etchant and wafer to form
etch-product
Desorption of etch-product form the
wafer surface
Acceleration of desorption of etch-product by ion bombardment
Transport of etch-product to the bulk
plasma
Redissociation of etch-product in theplasma or pumped out
Redeposited on the reactor wall or
pumped out
cf) If any of these steps fails to occur,
the overall etch cycle ceases and the step
failed is a rate-limiting step
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7. 4. 3. Radicals in plasma
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Nanophotonic semiconductor Materials Lab.11
Radicals are generated through dissociation and ionization
ex) e + O2 O+ + O* + 2e,
e + CF4
CF3+
+ F* + 2eRadicals are much more abundant than ions in plasma because;
(1) They are generated at a higher rate due to;
- lower threshold energy and ionization is often dissociative
(2) Radicals survive longer than ions
Although the concentration of radicals is much larger than that of
positive ions, the reactive fluxes incident on the surfaces can be
comparable, since ions are moving faster because they have
large energy obtained from the electric field in the sheath.
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7. 4. 4. Volatility and evaporation
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Nanophotonic semiconductor Materials Lab.12
Volatility of etch-products is a key distinction between plasma
etching and sputtering.
In general, desorption is a rate-limiting steps in the plasma
etching Highly volatile by-product formation is important.
Evaporation rate of material (a) of molecular weight Ma is
proportional to its vapor pressure, pa, (refer to Chap. II)
The evaporation rate is increased with increasing temperature.
However, plasma etching generally done at room temperature.
formation of volatile product at RT is most important.
RTHa
aa
RTH
aaaa
a
eRT
M
C
eCppRT
M
=
=
=
2
1
2
1
2
,2
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Boiling point of etch product (Si and metal)
K - JISTK - JISTMaterials Science & Engineering
Nanophotonic semiconductor Materials Lab.13
Etch product Boiling point() Comment
Si
(SiO2, Si
3N
4)
SiH4
-111.6 Gas at RT
SiF4
-95.7 Gas at RT
Si2H
6-15 Gas at RT
SiHCl3
31.7
SiCl4
56.7
Si2OCl6 135.5Si
2Cl
6147
Metal
(Ag, Al, Ti, Au, Co, Cr, Cu, Ni,
Pb, Pt, Ta, W, Zn)
AgCl 1550
AlCl3
182.7 Sublimation
TiCl4
136.45
TiF4
284 Sublimation
Au2Cl3 - Non volatileAu
2Br
3- Non volatile
CoCl2
1050
CrO2Cl
2117
Cr(CO)6
151
CuCl2
655 Non volatile
CuBr2 900 Non volatileNi(CO)
4-25
PbCl2
954
PtF6
69.1
TaF5
229.5
WF6
17 Sublimation
(CH3)2Zn 46ZnCl2
756 Non volatile
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Boiling point of etch product (III-V semiconductor)
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Nanophotonic semiconductor Materials Lab.14
Etch product Boiling point() Comment
III-V semiconductor
(GaAs, InP, GaN)
Ga2H
6-63 Gas at RT
GaCl3
201.3
GaCl2
535
GaF3
~ 1000
GaBr3
279
GaI3 < 345(CH
3)
3Ga 55.7
(C2H
5)3In -32 Gas at RT
(CH3)3In 88
InCl3
418 Sublimation
InBr3
371 Sublimation
AsH3 -54.8 Gas at RTAsF
5-52.9 Gas at RT
AsF3
63
AsCl3
130.4
AsBr3
221
PF3
-101 Gas at RT
PH3
-88 Gas at RT
PF5 -75 Gas at RTPCl
562
NCl3
< 71
NF3
-129 Gas at RT
NI3
- Explode
NH3
-33 Gas at RT
N2 -196 Gas at RT(CH3)
3N -33 Gas at RT
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Typical gases used for plasma etching
K - JISTK - JISTMaterials Science & Engineering
Nanophotonic semiconductor Materials Lab.16
Feed gas Mechanism Selective to
n type Si
Cl2
Chemical
SiO2
Cl2/C
2F
6Ion-inhibitor
SiCl4
Si
Cl2
Ion-energetic SiO2CCl4/O2
SiCl4/O
2
Al
Sl2/SiCl
4
Ion inhibitor
/energetic
SiO2, some resist,
Si3N4
Cl2/CCl
4
Cl2/CHCl
3
Cl2/BCl
3
III-V semiconductor
Cl2
Chemical
SiO2, resist
Cl2/BCl
3
Ion-inhibitor
Cl2/CH4
Cl2/CCl
4
CCl4/ O
2
SiCl4/O
2
III-V semiconductor
Without Al
Cl2/O
2Chemical Al-containing alloy,
SiO2CF2Cl2 Ion-inhibitor
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7. 5. Dry etch method and reactor type
K - JISTK - JISTMaterials Science & Engineering
Nanophotonic semiconductor Materials Lab.17
7.5.1. Dry etch method
Plasma method
(a) Plasma etching (PE)(b) Reactivel ion etching (RIE)
(c) High density plasma etching: Electron cyclotron resonance
etching (ECR) and inductively coupled plasma etching (ICP)
Ion beam method
(a) Ion beam etching (IBE)
(b) Reactive ion beam etching (RIBE)
(c) Chemically-assisted ion beam etching (CAIBE)
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Detailed characteristics of dry etching technique
K - JISTK - JISTMaterials Science & Engineering
Nanophotonic semiconductor Materials Lab.18
Parameter PE RIE MERIE ICP ECR IBE
(sputter)
frequency 13.56MHz 13.56MHz 13.56MHz 13.56MHz 2.45GHz -
Pressure
(torr)
0.1 ~ 10 0.01 ~ 0.1 0.010.001
~ 0.01
0.001
~ 0.01
0.001 ~ 0.1
Te (eV) ~ 8 ~ 8 ~ 5 ~ 4 ~ 4
Plasma
density~ 3e8-3 ~ 1e10-3 ~5e10-3 ~5e11-3 ~5e11-3 -
Wafer
location
Grounded
electrode
Powered
electrode
Powered
electrode
Powered
electrode
Powered
electrode
Powered
electrode
Ion voltage25 ~
100 V
250 ~
500 V
400 ~
1000 V
0 ~
1000 V
0 ~
1000 V
500 ~
2000 V
Ion energyNot
Controllable
Not
Controllable
Not
controllableControllable Controllable Controllable
Chemical
reaction
Yes Yes Yes Yes Yes No
Physical
reactionNo Yes Yes Yes Yes Yes
Selectivity Excellent Good Good Good Good Poor
Anisotropy poor Good Good Good Good Excellent
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Comparison of dry etching technique
K - JISTK - JISTMaterials Science & Engineering
Nanophotonic semiconductor Materials Lab.19
advantage disadvantage
RIE economicalslow etch rate,
plasma damage
CAIBE
Relatively fast etch
rate low versatility
ECR fast etch ratehigh price,
low scalability
ICP fast etch rate,low plasma damage
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7. 5. 2. Reactor types of dry etch
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Nanophotonic semiconductor Materials Lab.20
(a) Plasma etching (PE) and Reactive ion etch (RIE)
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K - JISTK - JISTMaterials Science & Engineering
Nanophotonic semiconductor Materials Lab.21
Plasma etching (PE) Same reactor geometry as PECVD system
Low ion bombardment energy due to the low sheath voltagedrop sample was loaded on the grounded electrode (anode)
Mainly chemical reactions and negligible physical etching
Isotropic etch profile
At relatively high pressure: 0.1 ~ 10 TorrReactive ion etch (RIE) Combination of chemical activity of reactive radicals with
physical effects due to high sheath drop sample was loaded
on the powered electrode (cathode) Ion bombardment strongly enhances the chemical process
Anisotropic etch profile due to ion bombardment
Lower operation pressure of 0.01 ~ 0.1 Torr
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Nanophotonic semiconductor Materials Lab.22
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(b) Magnetically enhanced reactive ion etching (MERIE)
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Nanophotonic semiconductor Materials Lab.23
Reduce the plasma loss on the chamber wall using magnetic field byelectromagnet bucket
Electron collisional efficiency increase by interaction of E and B field
Substrate rotation for uniformity increase
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(d) Inductively coupled plasma
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Nanophotonic semiconductor Materials Lab.26
13.56 MHz currents pass through ICP coil
RF magnetic field formation along z axis
Induction of vortex electric field
Electrons oscillation
Increase of electron collision efficiency
More effective plasma generation than
conventional RIE high radical density
Electrostatic shield configuration eliminates
capacitive coupling
Independent ion energy control by table
power
Z
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Types of Inductively coupled plasma
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Nanophotonic semiconductor Materials Lab.27
Cylindrical type ICP
Contamination-free geometry
Planar type ICP
Contamination of wafer by
sputtering of window material.
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Nanophotonic semiconductor Materials Lab.28
Laser interferometer on chamber-top
Optical emission spectroscopy throughsidewall window
Electrostatic shield btw quartz and coil
ICP/PECVD cluster tool in K-JIST
Inductively Coupled Plasma in K-JIST
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(e) Ion beam-based reactor
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IBE inert gas ion (Ar+) formation in
external RF ion source and extracted
to the reaction chamber by
acceleration electrode (grid).RIBE reactive gas besides inert gas
ions are extracted from the external
source to the reaction chamber. Etch
rate is increased by the additionalchemical reaction
CAIBE inert gas ion (Ar+) are
extracted from the external sourceand the reactive gas are
independently supplied to the wafer
surface through shower-ring just
above the wafer.