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Technology Excellence for Specialty Markets(and Etching Basics)
CorporateIntroduction
Semiconductor Equipment Manufacturing
USA manufacturingFocus on high growth specialty marketsLab-to-Fab solutionsMultiple production facilitiesISO-9000/9001
Plasma-Therm, Florida, USA Rev-Tech, Florida, USAAdvanced Vacuum Lomma, Sweden
Relocated toSt. Petersburg, FL
Plasma-Therm long history of excellence
1975 1990 20001974
Origin:RF power supplies
Acquired by
2009
Industry first single wafer production plasma etch reactor
First ever Photomask plasma etch system introduction
1983 1994
Incorporated
Privately owned and operated company
with headquarters in USA
Critical machining capabilities
2010 2011 2013
Industry first Plasma dicing
System in production
Product Line extension
3
2014
Etch and Deposition Solutions Leveraged Across Markets and Materials
Photonics FailureAnalysis
R&DPowerMEMSNEMS
SolarSolidState
Lighting
Wireless DataStorage
Adv.Photomask
&Imprint
Etch Solutions: ICP, RIE, PE, PHF-RIE, DRIE
Deposition Solutions: PECVD, ICP CVD
Plasma Dicing Solutions
Configuration FlexibilityFrom Lab to Fab
Single wafer Cassette-to-cassette
Open Fab IntegrationClusterLoadlock
Product Innovation
Singulator™VERSALINE®
Mask Etcher®LAPECVD™
Etchand
Deposition
Advanced Vacuum product lineupOpen load and single wafer loadlock
Vision 300 Vision 400 Apex SLR
Americas (St. Petersburg, FL)Sales and Service distributed throughout the US.1 Spares warehouse location
Supporting Over 640 Customers Worldwide
Asia-PacificJapan, China, Taiwan, Australia, Indonesia, Korea, Singapore, India, Malaysia4 Spares warehouses
EMEA France, Germany, Ireland, United Kingdom, Sweden, Israel, South Africa1 Spares Warehouse
13
Customer Recognized Service and Support
Global service organization operating 24/7Customer recognition of leadershipVLSIresearch 10 BEST/THE BEST Awards for 17 years2015 RANKED 1st in Etch & Clean Equipment Suppliers
9
Etching Basics:PlasmaReactorsMechanisms
2015
Mask
Etch Process
Etching: creating faithful reproduction of a pattern
Plasma Etching:Fundamentals, Mechanisms, Applications
Wet vs. DryWhat is plasma?Hardware/reactors overviewBasic Low-Pressure Processes
PhysicalChemical etchingIon driven etching, Ion enhanced etchingIon enhanced + Inhibitor (sidewall passivation)
Trends and TradeoffsPowerTemperaturePressure
Etching
Wet Dry
Ions Neutrals/Radicals
11
Why all the Focus on Dry Etching?What’s Wrong with Wet Etching?
Disadvantages
Limited CD geometry and control
Isotropic and/or crystallographic
Requires rinse and dry steps
Hazardous or toxic chemicals
Resist/wafer interface failure (undercutting)
Potential contamination sources
BenefitsPurely chemical
No physical damage
Can be highly selective
Wide choice of chemicals
Can etch many materials
Low capital cost
vs.
3
Plasma Basics: Why Pursue Dry Etching?
Many materials can be wet etchedAnd plasma……
requires a lot of technology to make it workinvolves many environmental health and safety aspectsis expensive
But plasma can do things wet can’tLess reactants requiredHigher purity reactantsLower contamination riskCompatible with other dry processes
Anisotropic Etching (Isotropic possible)Pattern smaller geometriesImproved CD control
Directionality: Pattern fidelity13
Plasma Basics:What is a Plasma – Tornado in a Trashcan?
Chemical “soup” , 4th state of matter
Neutrals Ions Electrons
Overall charge quasi-neutral
Most molecules/atoms not ionized
Non-equilibrium, constant creation/loss of species
Plasma electrons - small mass move fast ~9 x 10-28g
Plasma ions - big mass move slow
Plasma neutrals - big mass move slowDynamic!
14
Plasma Basics: How to make a plasma?
Add enough energy to a gas to cause ionizationElectricalThermalOther – e.g. electro-magnetic energy (radiation)
Low PressureNeon sign
Very low pressureInter-stellar space
High PressureLightningElectric welding arc
15
Plasma Basics: What is an Ion?
Ne
Ne+ + e-
+
10 protons 10 electrons (2 + 8)Charge balanced
10 protons 9 electrons (2 + 7)Extra positive charge
IonAtom
EjectedElectron
Simplified view
e-
Electron
Impact
Plasma Basics: Formation of Radicals by Electron Impact (e.g. Cl2)
Cl2 Cl + Cl
Electron
Impact
Charge balancedHappy to share an electron
Full outer shell
Neutral but “unhappy”Hungry to have just one more electron
to complete the outer shell
+
Cl RadicalsCl2 Molecule
e-
Simplified view
ne= electrons concentration
no= neutral concentration
ni+ = positive ion concentration
f(E) = distribution of energy
= residence time
excitation power
excitation frequency
gas flow rate
nature of gas pumping speed
chamber design
Plasma Basics: What makes up plasma?Focus on RF Generated Plasma
7
Plasma Basics: Simple Plasma Processes
Ion productionX + e- → X+ + e- + e-
DissociationAB + e- → A + B +e- (formation of neutrals and radicals)
Ion loss mechanismsX+ + e- → X (unlikely)X + e-→ X- (electron attachment, e.g. SF6)
X+ + wall (e-) → X (a major ion loss mechanism)
Light emissionX + e- → X* + e- (excitation)X* → X + h (photon emission)
Emission at specific energy (wavelength)
19
Many more process than those shown
Used for endpoint
Throttle Valve(controls pressure)
Basic Vacuum Processing System
Pressure (Torr, mbar) Volume (l, cm3, ft3)
Pumping Speed
PlasmaProcessModule
TurboMechanical
Pump
PressureGauge Feedback
Input
Exhaust
MFC = mass flow controller
We’ll talk about plasma a bit later…
MFCMFC
Gas Flow
Loadlock
20
Throttle Valve(controls pressure)
Basic Vacuum Processing System
PlasmaProcessModule
PressureGauges
Feedback
Exhaust
MFC = mass flow controller
We’ll talk about plasma in just a minute…
MFCMFC
Gas Flow
TurboMechanical
PumpLoadlock
Slot valve
21
PressureGauge
Plasma Basics: Equipment Configuration
NeedLow pressure
Gas
Electrical energy
Generator - Power source
Matching Network (to be discussed later)
Minimizes reflected power
Increases power dissipation in the discharge
Protects the generator
Acts as blocking capacitor
22
Blocking Capacitor
Plasma
RFGenerator
MatchingNetwork
Plasma Reactors:Low Density Plasma Sources
23
RIE is a confusing name –uses plasma (reactive species, ions)
RIE technology includes other configurations
RIE is a specific configuration (|| plate)RIE = CCP
ICP = RIE ICP
PE = Plasma Etching
MatchingNetwork
RF
Pump
Gas Inlet
CCP = RIE = Reactive Ion Etching
RFMatchingNetwork Pump
Gas Inlet
PoweredElectrode
Only one RF supplyNo independent control
of ions and radicals
Summary Etching is a Balance(ICP is a Good Compromise)
Neutrals - Chemical
Chemical controlled with ICP power
Ions - Physical
Physical controlled with substrate bias power
Inhibitors complicate the balance24
Plasma Reactors:High Density Plasma Sources
25
B
Magnetically Enhanced
MERIE ECR
ICP
TCP
Two RF suppliesMore control of ions and radicals
Plasma Etching Processes
Many simultaneous processesModeling gas dynamics, electromagnetics, reaction kinetics, surface interactions, etc.
Excellent references to the study of plasma etching
Plasma Etching: Fundamentals and Applications, M. SugawaraHandbook of Plasma Processing Technology, edited by S. Rossnagel, J. Cuomo, and W. WestwoodPlasma Etching: An Introduction, D. Manos and D. Flammhttp://www.chm.bris.ac.uk/~paulmay/misc/msc/msc1.htmD. Flamm, Pure & Appl. Chem., Vol. 62, No. 9, pp 1709-1720, 1990
26
Source: Oehrlein and Rembetski
Sputter Etching (“physical” etching)
High energy ions impact substrate surface and eject material -billiard ball effect
Yield/Etch Rate typically decreases with increasing process pressure
Etch Rate typically highest at low pressure (mTorr)
Ion
Sputtering
27
Sputter Etching
Characterized by non-volatile byproductsFluorine based chemistry (e.g. LiF, CaF: tungsten, titanium,, silicon)Chlorine based chemistry (CuCl2)No easily made byproducts (e.g. gold, platinum)
High bond energies (e.g. GaN, Al2O3), characterized by low selectivity
28
- Sputter etch
- Unknown- Etchable at RT
- May be able to etch
- Gaseous
H
Li Be
Na Mg
K Ca
Rb Sr
Lu
Y
BaCs
Sc
Ta
Cd
Ir
Rh
Co
OsW
TcMo Ru
Fe
Hf
Nb
Re
Mn
Zr
CrVTi Zn Ge
Si
FN Ne
ClS
Au
Al
C
Pb
O
Se
Ar
Rn
Te
Pt Hg
Ga
B
Sn
P
KrBr
Pd
Ni
Ag
Cu
Tl
In
Bi
As
Sb
He
At
XeI
Po*
1/IA
2/IIA
3/IIIB 4/IVB 5/VB 6/VIB 7/VIIB 9 10
VIIIB
13/IIIA
12/IIB11/IB
18/VIIIA
17/VIIA16/VIA15/VA14/IVA
8
Sputtering Process
Ions create a cascade of collisions on the surface.
Multiple collisions eject (or 'sputter') atoms from the surface.
Sputter yield depends on :Target material (how tightly bound and density)
Incoming ion mass (typically Ar, He too light, Xetoo expensive, hard on turbos)
Energy of the incoming ion
29
Material SputterYield*
Silver 3.4Gold 2.8
Copper 2.3Platinum 1.6
Nickel 1.5Iron 1.3Al 1.2Si 0.5
Al2O3 0.05
*600 eV Ar ions Source: Angstrom Sciences
www.angstromsciences.com/ref.sputtering-yields
Note: Si has very low sputter yield, so does graphite
Sputter Etching – Purely physicalCommon Reactor Configuration
“RIE” mode (common configuration)
Sputtering mode with inert gas (usually Ar)
Low etch rates but can remove non-volatile materials
Profile may be directional (but rarely vertical)
Ion energy, flux and radical conc. not independent
Low selectivity- most materials sputter equally
Mask choice is important but not always a problem. May produce desired result
“Dirty”– Process products not volatile and accumulate on chamber and feature surfaces
Typically 13.56 MHz
Inert Gas (e.g. Ar)
SubstrateRF
MatchingNetwork
CapacitivePlasma
30
Angular Dependence of Sputter Yield
Results in enhanced etch rate at angle of max. value (θmax)
Etch profile will develop at this angle
“faceting” of mask
Angle (degrees)0 90
Max. sputter yield angle
31
θmax
Spu
tter R
ate
θmax
Substrate
Sputter Etching and Development of Sloped Etch Profile
As mask material is sputtered away it preferentially is lost at the corner (some part of the corner equals θmax)
32
Example: resist after etching
Not perfectly 90° at corner
CD loss
Angle approaches angleof max. sputter rate
θ
Resist erosion
Sputter Etching: Mask Profile Can Affect Feature Profile
Lateral erosion of resist mask can cause feature size shrinkage or roughness
33
GaAs
Photoresist
Another description is that forward sputtering will always round a corner
Silicon
Photoresist
SiC
Oxide
Angled ProfileSometimes it’s not a problem, it’s a solution!
Starting resist profile
Desired result (patterned sapphire for LED manufacturing
Beginning of mask faceting
Mask slope transferring to feature
34
Sloped Masks Make Vertical Etching Difficult
Selectivity = ERmask/ ERfilm = tan(θfilm)/tan(θmask)Use to predict slope.
35
Selectivity Mask θmask Best Profile1 75 75.01 80 80.01 85 85.02 75 82.42 80 85.02 85 87.53 75 84.93 80 86.73 85 88.3
10 75 88.5
Sputter Etching: Can create “grass” or sidewall redisposition
Micro-maskingOften redeposited mask materialDepends on mask material, bias, ion massTends to be less farther from masking material
Not the only source of micromasking (e.g. excessive passivation, to be discussed later)
36
37
Sidewall redepositionGold Etching – Process Example
Gold
PRRe-sputter
“Dog ears”After mask removal
After “etch”
Sputter Etching: Can be a source of “trenching”
Deflected ionsIncreased etch rate at mask edgeDepends on mostly on bias and ion mass
38
Bias Power200 W 250 W 300 W
Chemical Etching
Dominated by neutral reactive species (atoms, radicals, molecules)
Radicals react with film surfaceReaction is spontaneous – ion assistance not required
Purely isotropic (nondirectional) and low damage
Reaction by-products are volatile
Volatile ProductNeutral
Chemical Etching
39
Etch Product Volatility Guidance
40Source: C. Cardinaud et.al., Applied Surface Science 164, pp72-83 (2000)
Chemical Etching: Common Reactor Configurations
CCP = RIE= Reactive Ion EtchingLower electrode poweredRun at low power to avoid
unwanted sputtering
PE = Plasma EtchingUpper electrode powered
RF + MatchPump
Gas Inlet
Pump
Gas Inlet
RF + Match
ICP = Inductively Coupled Plasma Etching
Substrate bias and highdensity plasma
41
Gas Inlet
RF + Match
RF + Match
Low density plasmas
High density plasmas
Chemical EtchingReactor Configuration
PE configurationLittle ion bombardment – almost “purely” chemical etchLeast flexible configuration
RIE = CCP configurationHigh pressure operation to minimize ion reactions Low plasma/radical density (low etch rates)RF power/ion bombardment not independent
ICP configurationHigh plasma/radical density (high etch rates)Can operate with no bias – almost purely chemical etchPlasma density/ion bombardment are independent
42
Low density plasmas
High density plasmas
Chemical Etching: Examples
Spontaneous etch reactions (examples)Si with SF6 (F radical)SiNx with SF6 (F radical)GaAs with Cl2 (Cl radical) (Interestingly NOT etching Si with Cl2)Al with Cl2 (Cl radical)HC polymers (e.g. PR) with O2 (O radical)
Choice of chemistry can provide high selectivitySiNx/SiO2 using SF6
GaAs over InGaAs or AlGaAs using Cl2
43
Chemical Etching: Examples
Silicon pillar, SF6
GaAs, HCl(crystallographic)
Silicon trench, SF6
InP, HBr
GaAs, Cl2
44
GaAs, Cl2
Chemical Etching: Characteristics
45
High etch rates possibleHigh radical concentrations possible in plasma (particularly ICP)
Higher density at higher pressureRate limited by mass flow balance (what goes out, must come in)
Load dependent etch rateEtch rate lower as etched area increases
Consequence of mass flow balance
Frequently classic “bulls-eye” uniformity profileEdge of substrate etches faster than center
Same # radicals at substrate edge but less area
Chemical Etching: Edge Effect
Edge has less area for available reactant
flux
substrate
film
Etc
h ra
te
Center EdgeEdge
Gas Phase Reactants
46
Chemical Etching: Reduction of edge effect
Other solutions:High pump speeds, dilution
substrate
film
Gas Phase Reactants
Etc
h ra
te
Center EdgeEdge
substrate
film
Physical barrier limits speciesaccess to edge
47
uncorrected
corrected
Modest changes in gas phase chemistry can have strong impact on etching
In this case, adding ~15% O2increases etch rate ~4xSi + F → SiFx
Chemical Etching: Controlling Reaction Kinetics
Formation of F: CF4 + e- → CF3 + F + e-
(electron impact) CF3 + e- → CF2 + F + e-
Radical recombination: CF3 + F → CF4(loss of F) CF2 + F → CF3
Addition of O2: CF2 + O → COF + F(generation of F) COF + O → CO2 + F
Si R
elat
ive
Etch
Rat
eO2 %
10 20 30 40 500
0.2
0.4
0.6
0.8
1.0
060
Relative F Intensity0.2
0.4
0.6
0.8
1.0
0
703.7 nm line intensity(F etching Si)
Silicon etch rate
Addition of O2 to CF4
Source: C.J. Mogab, A.C. Adams, D.L. Flamm, J. Appl. Phys. 49, 3796 (1978)
48
Chemistry Choice - Volatility of By-product(s)
49
Source: T.P. Chow, A.J. Steckl, Electron Devices, IEEE Transactions, 11, 1983
Refractory metals and silicides
Chlorine based
Log
10P
(m
m)
Fluorine based
Fluorides ChloridesAlF3 1291 AlCl3 178 sub
Cu2F2 1100 Cu3Cl3 1490TiF4 284 TiCl4 136WF6 18 WCl6 347
Use vapor pressures when available or boiling points as a guide when they
are not
Chemistry Choice - Volatility of By-product(s)
Chemistry Primary Films Etched
Cl – based ( e.g. Cl2, BCl3, SiCl4) Al (+ alloys), Ti, TiN, W, Cr, Hf, W, Mo
F – based (e.g. SF6, CF4, CHF3) Ti, W, TiW, WN, Mo, Ta, silicides
50
Other factors play a role:• masking materials• additive gases, • film quality,• desired results,• etc.
Physical and chemical components: individually slow but together increase the etch rate and anisotropy
Combination of radicals and ions etch wafer
Ions striking the surface enhance reactions and product desorption
Ion Enhanced Etching
Ion Enhanced
ProductIon
Neutral
51
Ion Enhanced Etching:Common Reactor Configurations
RF + MatchPump
Gas Inlet
Gas Inlet
RF + Match
RF + Match
CCP = RIE configurationLow pressure operation to maximize ion formation Low plasma/radical density (low etch rates)Ion density/ion energy not independent
ICP configurationHigh ion densityPlasma density/ion bombardment are independent
ICP power → ion and radical densitiesBias power → Ion energy
52
Ion Enhanced EtchingExperiment shows role of ions/radicals
Illustrates the dramatic affect of combining radicals and ions
Source: J.W. Coburn, H.F. Winters, J. Appl. Phys. 50, 3189 (1979)
XeF2 gasonly
Ar+ ion
beam
XeF2gas+
Ar+ ionbeam only
> 10x etch rate increase
ModelsReactive spot (energy addition)
Tachi (1985)Damage & enhancement
Coburn & Winters (1978)
53
Radicals Radicals + Ions Only Ions
spontaneous
Ion enhanced
sputtered
Other early studies of ion effects
Al with Ar+ + F2Low volatility of AlF3 , Al alone sputters faster
Si etching with Ar+ CF4CF4 is not adsorbed on Si surface
Si etching with Ar+ Cl2SiCl4 volatile
Source: J.W. Coburn, H.F. Winters, J. Appl. Phys. 50, 3189 (1979)
Source: J.W. Coburn, H.F. Winters, J. Appl. Phys. 50, 3189 (1979)
Source: Pabst et al., Int. J. Mass Spect. Ion Phys. 20, 191 (1976)
54
Ion Enhanced EtchingIons contribute to anisotropy
Example: XeF2 etching of Si
Anisotropy 1
Higher anisotropy with higher energy ions
Penalty for anisiotropy by increasing ion flux or energy –but typically lower selectivity, trenching, damage
55
Source: P. Martin, Vacuum Technology & Coating, , 28, (Nov. 2009)(Not the original reference)
XeF2 Flow rate
Ion Enhanced Etching Examples
GaN with Cl2: ions assist desorption of GaClx etch products
SiC with SF6: ions assist formation of SiFx and CFx etch products
SiO2 with CF4: ions assist formation of Si and C etch products
Al2O3 with BCl3: ions assist formation of AlClx etch products
56
Ion Enhanced Etching
Ion bombardment is necessary to break strong bondsSi – O 8.2 eVAl – O 9.3 eV
By products must still be volatile (e.g. SiF4, AlCl3)
Vertical ion bombardment →vertical etchMask erosion may result in sloped profile (similar to sputter etch)
Choice of radicals can provide selectivitye.g. etching SiO2 with CF4 (CF2 and CF3 radicals)Selectivity less than Chemical etch and greater than Sputter etch
Loading effects < chemical etchRate rarely mass flow limited
57
Ion Enhanced Etching + Inhibitor(Sidewall passivation)
Inhibitor (often polymer forming) can passivate surfacesMinimal ion bombardment on sidewalls to remove inhibitorSurface protected from etching
Passivation removed from horizontal surfaces by ion bombardmentSurface open for etching (chemical or ion assisted)
ProductIonReactant
Inhibitor
Inhibitor
58
undercut
Most highly anisotropic processes fall in this category
Inhibitor introduced intentionallySi etch using SF6 plus C4F8 Al etch using BCl3/Cl2 plus CH4InP etch using HBr or Cl2 plus N2
Inhibitor introduced “unintentionally”Etching using photo resist mask
Resist etch by-product is polymer precursorEtch result depends on resist loadingAnisotropic etch with resist mask, isotropic with “hard” mask
e.g. GaAs via etch with resist mask
Ion Enhanced Etching + Inhibitor
Source: after M. Mieth and A. Barker, Semiconductor International, 5, 222 (May, 1984)
59
Materials which act as inhibitors
Photoresist etch by-product (particularly from Cl etch)
Hydrocarbons e.g. CH4
Chlorinated hydrocarbons e.g. CHCl3 (most banned)
Freons
CHF3 ~= C4F8 > C2F6 > CF4
F:C ratio and oxidation capability of surface determines effectiveness as polymer precursor (e.g. O from SiO2 can provide oxidation source)
N2 for some processes, e.g. Al, InP
O2 can oxidize sidewall e.g. silicon (e.g. cryo black silicon process)
60
Ion Enhanced Etching + Inhibitor
Isotropic etch induced notch in feature profile
HBr/CH4/BCl3Preferentially etches InGaAs layer
HBr/N2Inhibition of InGaAs etching
Example: Multilayer InP/InGaAs/InP
61
Requires understanding of how inhibitors participate(e.g. CH4 sometimes an inhibitor, sometimes an etchant
Ion Enhanced Etching + Inhibitor
Anisotropic GaAs etch (via etch) using Ar/Cl2Resist by-products provide sidewall passivation
Polymer provides sidewall protection
62
GaAs Profile Control- Isotropic to Anisotropic
Selectivity increases with Cl2 partial pressure: etch rate and isotropy increases
Resist implicated in controlling profile
63
Cl2 partial pressure (mTorr)
GaA
s Et
ch R
ate
(um
/min
)
Etch Selectivity (GaA
s:PR)
40 um vias
Tungsten Etch Example
Beforeetch
SF6 / CF4 / Ar
F for reaction, CF4 for passivationVertical profile
Sidewall roughness transferred from mask roughness
PR
Al
W
Al
W
64
Afteretch
Process temperature 20CSelectivity to PR ~5:1
~2000 A/min
Tungsten Etching with Fluorine Chemistry
Source: Tang and Hess, J. Electrochem. Soc. 131, 115 (1984)Mark Salimian, Plasma Etching, Technologies and Processes, 1993
CF4 / O2 vs. SF6 / O2: Etch rate and Relative F Atom Density• F is primary etchant (similar activation energies) for SF6 and CF4
• O2 increase rate for CF4 /O2 with more available F. O and F compete for W sites• O2 decrease rate for SF6/O2 , interaction with SFx and W? (adding O2 doesn’t help)
Etc
h ra
te (n
m/m
in)
Rel
ativ
e F
Ato
m D
ensi
ty
(arb
. Uni
ts)
Rel
ativ
e F
Ato
m D
ensi
ty
(arb
. Uni
ts)
Etc
h ra
te (n
m/m
in)
CF4 / O2
SF6 / O2
65
Mask material is often important
RIE with SF6
PRSiO2W
PRSiNxW
SiO2W
SiNxW
Data suggests O from SiO2 attacks sulfur (S) protection layer on W
More efficient removal of inhibitor than N from SiNx
Source: Sato et al, 7th Plasma Process Symp. Proceedings Electrochem. Soc. 1988, p240Source: Mark Salimian, Plasma Etching, Technologies and Processes, 1990
66
Often involved in achieving anisotropic profilesBalance of etchant and inhibitor
Profile, uniformity sensitive to ratio Too little inhibitor, profile → isotropicToo much inhibitor, etch rate decreases, polymer formation, micro-masking
Balance can change with Aspect ratio (mass transfer issues)Temperature sensitive
Polymer deposition (affects profile) changes with temperaturePotential for deposition on chamber surfaces
Reduced at elevated temperatures
Ion Enhanced Etching + InhibitorCharacteristics
67
Excess inhibitor deposition causing grass
Al Etch – General Considerations
Typical Al process steps:Breakthrough (remove native oxide) → Main etch → Post etch treatment
Material composition issuesAl-Si: Si residues may require post F-plasma treatment (e.g. CF4) to remove unetched Si (this may impact underlayer)Al-Cu: Cu difficult to etch, susceptible to “grassing” from precipitates
Requires higher temperature and more ion bombardment Cu3Cl3 a temperature of about 200C
Al deposition quality: no O2 present Reduce Al2O3 formation during deposition: no leaks, loadlock, high purity Ar
Al2O3 formation from poor vacuum conditions (e.g. leaks, outgassing)Mask profile (sloped, rough, or poor adhesion)Corrosion (post etch)
68
Al EtchingAnother example of sidewall passivation
Photoresist erosion assists sidewall passivationResist condition (e.g. slope, bake temperature)
Surface AlCl3 reacts with moisture exposure to make HClwhich corrodes Al
Cl residues in resist & sidewall deposits also react to form HCl
TreatmentsIn-situ PR strip (O2 ash) (best)
F replacement of Cl using CF4 (O2) (possibly SF6)
CHF3 will deposit polymer protecting the wafer from moisture attack.
Immediate rinsing of wafer and removal of resist after Al etch
High temperature bake (usually not available due to PR)
Substrate
Al
Photo-resist
Sidewallfilm
Cl
AlC
O
69
Al Etching – BreakthroughRemoval of Native oxide
Surface reacts to ambient atmosphere to make 20-50Å Al2O3
Cl2 alone won’t work. Al2O3 + Cl2 → AlCl3 + O2 (makes more Al2O3)BCl3 to needed to reduce Al2O3
Al2O3 + BCl3 → AlCl3 + B2O3 (BOCl)BCl3 acts as an O2 scavengerCClx could be used but carcinogenic (Al2O3 + CClx (x ≤ 4) → AlCl3 + CO)
Even with reducing chemistry and energetic ion bombardment, the etch rate of Al2O3 is >300x less than Al
70
Al
A2O3
Cl Cl Cl Cl Cl Cl
Cl2Al + O2
Al
Al2O3
Cl Cl Cl
Al
Surface oxide Surface reoxidized
Al Etching – Main Etch
Al (unlike Al2O3) can be etched in Cl2 (or with BrCl2 reacts spontaneously at RT (without plasma or ion bombardment)
AlCl3 sufficiently volatile at 20C to desorbDesire high pumping speed (low residence ) reduces AlCl3 partial pressureHeated chamber walls (reduce re-deposition)Load lock (safety and low oxygen presence)
Highly load dependent (chemical component) may require diffusion barriers to improve uniformity)Al not etched in F-containing gases. AlF3 only volatile at elevated temperatures (i.e. chamber should be free of F)
71
Al
Cl Cl ClCl2
Cl Cl Cl
Al
Al
AlCl3 or (AlCl3)2
AlAl
Plasma EtchFeature Profile Defects
72
BowingMask Facet
TrenchingIon Reflection
UndercutUnder Passivation
TaperOver passivation
NotchingCharging
Re-entranceIon Scatter
Source: adapted from Donnelly, V. M. and Kornbilt, A., J. Vac. Sci. Technol. A 31, 050825 (2013).
Tilt-SkewIon Trajectory
Physical effects (ions)Mask facetingIon scatteringOff-angle ions
Chemical effectsOver passivationUnder passivation
Neutral beam solutions?
72
Damage EffectsProcess and device dependentMultiple types of damage can result from processes
Ion damage to lattice (e.g. ion penetration, vacancies, interstitials)
Carrier passivation (carrier concentrations)
Surface contamination (surface states) (e.g. fluorocarbon layers)
Recombination centers
Surface morphology
Insulator breakdown/leakage
Depth can be surprisingly deepSurface to many 100s Å
73
Many sources
Damage examples
H ion penetrates ~5x deeper
UV/VUV penetrates deeper with O2 plasma but fewer defects near surface
Source: Seiji Samukawa et al 2012 J. Phys. D: Appl. Phys. 45 253001
Source: Wong, Green, Liu, Lishan, Bellis, Hu, Petroff, Holtz, Merz, J. Vac. Sci. Technol. B 6 (6) 1906 (1988)
Buried Quantum Well Photoluminescence for Monitoring Etch Damage Depth
Damage ExampleInP Etching: RIE vs. ICP
CH4/H2 chemistry
75
RIE 2x P surface loss enhanced
RIE 2-3x thicker amorphous layer
RIE has lower etch rate
RIE P depleted layer ~2x ICP Source: Cardinaud, C, et al,., Appl. Surface Science, 164 (2000) 72-83
Summary - Etching Mechanisms
Volatile Product
Sputtering Ion Enhanced
ProductIon
Chemical
Neutral
Ion
Ion Enhanced + Inhibitor
Neutral
ProductIon
Neutral
Inhibitor
Inhibitor
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SummaryBasic Low Pressure Etching Mechanisms
Sputter EtchingIons strike surface and eject or sputter materialNonvolatile reaction products
Chemical EtchingNeutral dominated (atoms, radicals, molecules)Isotropic, non-directional, can be reagent limited
Ion Driven EtchingIons strike surface and enhance reactionsBoth physical and chemical componentsAllows “fast” anisotropic etching
Ion Enhanced + Inhibitor FormationPolymer forming components passivate sidewalls where ion bombardment is minimalPrevention of lateral etching
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Pressure EffectsStrong effects
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Ratio of sheath thickness and mean free path of ion
High pressure• Requires additional control
mechanism (e.g. passivation)• More neutral influence
Ion flux
Neutralflux
Ion flux
Neutralflux
Physical(sputtering)
1 10 100 1000
Ion
Ener
gy
Pressure (mTorr)
Ion Assisted(chemical and physical
Chemical(radicals)
Low pressure• Stronger ion influence• More directional (CD control)• Potential for more damage
Pressure EffectsStrong effects
Affects ion energy, density, bias, electron temperatureReduction in pressure increases electron temperature and this results in increase in DC bias (more electrons “leave” the plasma)
Chemical based processes – etch rate usually increases with pressure (longer residence time for reactants)
Ion enhanced processes – Etch rate might actually decrease with increasing pressure (lower ion energies)
Profile affected: mass transport (lag), sidewall passivation
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Power Effects
Increased ICP power increased concentration of radicalsIncreased electrode bias power increased DC bias
Increases the effect of ions (more energetic and more of them)Mask erosion increases selectivity decreases
Possible to actually have better selectivity if material of interest etch rate goes up faster than mask erosion
Wafer cooling becomes more important as either ICP or bias power increases
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Wafer gets hot with all the energy being delivered (and exothermic reactions)
Need to manage thermal budget!
Temperature Effects
Wafer temperature affects etch rate, selectivity, surface roughness and anisotropyChemical processes affected the most
Temperature , isotropy (and often roughness)Temperature , Etch rate Temperature , Selectivity (usually but not always)
Consider Si etching masked by SiO2 (example) RateF (SiO2) = 6.14 x 10-13 nFT1/2 e-0.163/kT Å/min RateF (Si) = 2.91 x 10-12 nFT1/2 e-0.108/kT Å/min Selectivity = RF(Si)/RF(SiO2) = 4.7 e +0.055/kT ( higher T, lower
selectivity)Changes in T can have large effect on selectivity (e.g. InP etching)
Photoresist etch rate increases with temperature
81Source: Flamm et al., VLSI Electronics, Vol. 8, Chap (1984)
General Process Trends
Response with Increase in Process Parameter
Process Parameter Etch Rate Selectivity(to mask)
Mechanism Trend Uniformity
Bias Power Increases Decreases More physical Weak effectElectrode Size
(power density) Decreases Increases Less physical Weak effect
Source Power Increases Increases More chemical Weak effect
Pressure Usually increases Weak effect More chemical Usually worse
Substrate Temperature Increases Depends More chemical Weak effect
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Important Caveat: material dependent
Advanced Plasma DevelopmentsInterest in removing ions & controlling neutral energies
ALE – Atomic Layer EtchingTemporalSpatial
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RF Bias
Source: adapted from Ankur Agarwal et. al., J. of Applied Physics, 106, 103305, (2009)
Neutral control –grids, ion filters
Pulsing ICP source
Pulsing bias
Multiple frequencies Pulsed gases
Temporal EtchingAtomic Layer Etching (ALE)
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Adsorb
Flush
Flush
Volatize
Time-Multiplexed EtchingAtomic Layer Etching (ALE)
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Source: Donnelly, V. M. and Kornbilt, A., J. Vac. Sci. Technol. A 31, 050825 (2013).
Potential BenefitsMonolayer control of etchElimination of profile defectsElimination of ARDE
LimitationsExtremely low etch ratesNarrow process window to achieve monolayer control
StatusDemonstrated in Si Cl-based chemistries4 step cycle demonstrated
280 ALE cycles150sec cycle times
Spatially Multiplexed EtchingDRIE
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Source: Roozeboom, F. et al., ECS Trans. 50 (32), 73-82 (2013).
Spatial ALD ReactorSpatial DRIE Approach
Summary Usually there are Tradeoffs
Etching Rate
Selectivity
Surface Morphology
Profile
DamageUniformity
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