advancing atomic layer deposition and atomic …...• ald-style gas dose delivery using “ald...
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Page 1© Oxford Instruments 2018
Advancing Atomic Layer Deposition and
Atomic Layer Etching
Harm Knoops, Oxford Instruments Plasma Technology
Page 2© Oxford Instruments 2018
• Structure:
• Miniaturization, more complex structures and more 3D
• Device:
• Lower damage, interface control
• Material:
• Wider range of tailored material solutions, lower thermal budget
Why are ALD and ALE gathering more interest?
GaN
buffer
AlGaN
Gate
substrate
source drain
Vorobyov et al., Opt. Mat. Exp. 7, 513 (2017)
GaN transistors Quantum devices Biosensing
Page 3© Oxford Instruments 2018
Generalized ALE/ALD cycle
Faraz et al., J. Solid State Sci. Technol. 4, N5023 (2015)
Page 4© Oxford Instruments 2018
Key features ALE vs. ALD
Faraz et al., J. Solid State Sci. Technol. 4, N5023 (2015)
Page 5© Oxford Instruments 2018
• Conventional etching involves continuous amorphisation of several
atomic layers and chemical reactions in that amorphised layer
• ALD and ALE provide control and low damage options to allow
minimal influence on sensitive surfaces.
Low damage for minimal influence top layers
From O. Joubert, SEMATECH Workshop on Atomic-Layer-ETch (ALET) and - Clean (ALC) Technology, April 21, 2014
Conventional etching ALE
Increasing ion energies
Page 6© Oxford Instruments 2018
• Why ALD and ALE?
• ALD
• Stress-control in oxides
• Low-resistivity nitrides
• Novel plasma gases
• ALE
• Processes
• Smoothening
• ALD and ALE
• Conclusion
Outline
Page 7© Oxford Instruments 2018
• Cutting edge plasma ALD systems with
thermal ALD as standard
• Mixed mode operation within a single recipe
• No hardware changes required to switch
mode between plasma and thermal ALD
• e.g. start with thermal Al2O3 on sensitive
interface but continue with plasma ALD
for best material properties
Oxford Instruments ALD
FlexAL
Page 8© Oxford Instruments 2018
• To limit etching of a polymer plasma
conditions can be set to reduce etching
• High pressure plasma allows growth on
polymers without etching them
• ALD deposit will also function as
protective layer, so generally etching is
minimal
Low damage for depositing on polymers
Rate of the resist removal during 50
plasma exposures of 5 s each
Page 9© Oxford Instruments 2018
Applying substrate biasing to enhance the ion energy
The FlexAL ALD system can be equipped
with table bias for extended process
capabilities (e.g., higher conductivity,
higher crystallinity, stress control).
• Up to 550 °C temperature.
• Up to 100 W RF power.
• 13.56 MHz
• Up to 500 V resulting DC bias.
• Fully automated RF matching.
Page 10© Oxford Instruments 2018
Material properties control by biasing
A wide range of properties can be tuned by substrate biasing in ALD
Faraz et al., ACS Appl. Mater. Interfaces 10, 13158 (2018)
Page 11© Oxford Instruments 2018
Potential usage in devices
• Stress control on planar surfaces for MEMS devices.
• Anti-reflective TiO2 coating with low stress.
• Al2O3/HfO2 higher-k dielectric.
• Ta2O5 barrier layer with specific stress.
• Conductivity and superconductivity control of TiN and
NbN for quantum devices. Faster deposition of high-
quality material expected with biasing.
• Resistivity/work-function/stoichiometry control for gate
metals (e.g., TiN, HfN).
Vorobyov et al., Opt. Mat. Exp. 7, 513 (2017)
Superconductivity control
Stress control
Page 12© Oxford Instruments 2018
Shestaeva
Shestaeva
Film stress in thermal and plasma ALD of Al2O3
• Stress decreases with deposition
temperature. Higher than
estimated from thermal stress.
growth related due to voids,
impurities or dislocations?
• Plasma similar material properties and
similar stress to thermal ALD. Ylivaara et al., Thin Solid Films 552, 124 (2014)
Shestaeva et al., Applied Optics 56, C47(2017)
Residual stress
Ohring, The Material Science of Thin Films, 1992
Page 13© Oxford Instruments 2018
Beladiya et al., Proc. SPIE 106910E (2018)
Faraz et al., ACS Appl. Mater. Interfaces 10, 13158 (2018) 0 50 100 150 200 250 300-3000
-2000
-1000
0
1000
2000
Compressive
Al2O
3
TiO2
SiO2
Resid
ual S
tress (
MP
a)
Average bias voltage (V)
HfO2
Tensile
Film stress as a function of biasing for ALD oxides
• Generally tensile without biasing.
• Typically more compressive with
bias up to certain voltage.
• Bias trends very dependent on
material.
Page 14© Oxford Instruments 2018
0 50 100 150 200 250 300-3000
-2000
-1000
0
1000
2000
Mixed
RutileAnatase
Monoclinic
Amorphous
Compressive
300 °C
TiO2
Resid
ual S
tress (
MP
a)
Average bias voltage (V)
150 °C
HfO2
Tensile
Relation of stress with crystallinity when biasing
• Crystallization can cause tensile
stress, further biasing generally
makes film compressive.
• Similar behaviour found for
Ta2O5, MoO3, and WO3.
Faraz et al., ACS Appl. Mater. Interfaces 10, 13158 (2018)
Page 15© Oxford Instruments 2018
Effect of bias duration for TiO2
0 100 200
-2250
-1500
-750
0
750
10 s bias
Average Bias Voltage (V)
Compressive
Re
sid
ua
l str
ess (
MP
a)
Tensile5 s bias
• ALD by TDMAT and 10 s O2 plasma at 300 °C.
• At 100 V near zero stress, for anti-reflective TiO2
coating with low stress.
Choosing bias duration can give additional control.
Precursor (A)
Purge
Co-reactant (B)
Source Plasma (RF-ICP)
Substrate Bias (RF-Bias)
Time
1 cycle 2 cycles
Faraz et al., ACS Appl. Mater. Interfaces 10, 13158 (2018)
Page 16© Oxford Instruments 2018
Effect of bias on plasma ALD TiN
• ALD by TDMAT and 10 s H2/Ar plasma at 200 °C.
• Tuning of crystallinity, resistivity, density, and
stress.
Faraz et al., ACS Appl. Mater. Interfaces 10, 13158 (2018)
Page 17© Oxford Instruments 2018
Effect of bias on plasma ALD NbN
• ALD by TBTDEN and 20 s
H2/Ar plasma at 250 °C.
• Similar trend as for other
conductive nitrides. Strong
correlation between film
resistivity and film stress.
• High superconducting
transition temperature of
12.9 K for ~45nm NbN film-4000
-3000
-2000
-1000
0
1000
2000
3000
0
100
200
300
400
500
0 15 30 45 60 75
Film
Str
es
s (
MP
a)
R.T
. R
esis
tivit
y (
µΩ
*cm
)
Bias RF power(W)
resistivity with 20s plasmaexposure
film stress on Si with 20s plasmaexposure
Tensile
Compressive
~40nm NbN films
Page 18© Oxford Instruments 2018
• Robust ALD Process: Self-limiting ALD growth over wide temperature
window, high GPC (0.1 nm/cycle), Oxygen and carbon free (<2%)
• Digital layer thickness control from mono-layer to few layer material
• Tunable morphology: Control over basal plane or edge plane orientation
• Potential applications: Nano-electronics and catalysis
FlexAL2D: Plasma ALD of MoS2
www.oxinst.com/FlexAL2D
Page 19© Oxford Instruments 2018
• AlF3 ALD using TMA and SF6 plasma in FlexAL.
• Refractive index of 1.35 at 633 nm.
Aluminium fluoride (AlF3) ALD
Conformal
coating of GaP
nanowire
Wide temperature window
and no growth delayLow absorption over a wide range
Vos et al., Appl. Phys. Lett. 111, 113105 (2017)
Page 20© Oxford Instruments 2018
• Why ALD and ALE?
• ALD
• Stress-control in oxides
• Low-resistivity nitrides
• Novel plasma gases
• ALE
• Processes
• Smoothening
• ALD and ALE
• Conclusion
Outline
Page 21© Oxford Instruments 2018
ALE configuration
• ALD-style gas dose delivery using “ALD valves”
with 10 ms open-close response.
• Low bias power control 0.3 W to 300 W or 600 W.
• Ability to operate as a standard etch tool or in fast
low power ALE mode. Mode selection via
software recipe control.
• Wafer clamped mechanically using
helium backside cooling.
Oxford Instruments ALE tool
Page 22© Oxford Instruments 2018
Reliable gas delivery: OES analysis of CHF3 pulses
Repeatable
dosing using
ALE hardware
Dosing using
conventional
gas box
0
200
400
600
800
1000
1200
1400
1600
1800
2000
460 480 500 520 540
C2O
ES
in
ten
sit
y
Time (secs)
MKS1179 MFC
ALE hardware: 45 and 74msecs
Sensirion MFC: valved then not
Valve
closedValve open Valve closed
0
5000
10000
15000
20000
25000
30000
35000
40000
0.00E+00 1.00E+02 2.00E+02 3.00E+02 4.00E+02 5.00E+02 6.00E+02
0
1000
2000
3000
4000
5000
6000
2.10E+03 2.15E+03 2.20E+03 2.25E+03 2.30E+03 2.35E+03 2.40E+03 2.45E+03 2.50E+03 2.55E+03 2.60E+03
ALE hardware provides short
burst of gas to the chamber
with no residual gas
Page 23© Oxford Instruments 2018
ALE Processing experience
Experience in processing materials
• Demonstrated results in a-Si, Si, SiO2, MoS2 ,
GaN, AlGaN layer etching.
• Collaboration with universities and institutes to
develop ALE recipes. ALEGRO project.
• Partnership with production manufactures to
develop solution for normally-off GaN HEMT.
Material Etched Dose Gas Etch Gas
Si or a-Si Cl2 Ar
MoS2 Cl2 Ar
SiO2 CHF3 or C4F8 Ar or O2
AlGaN/GaN Cl2, BCl3 Ar
AlGaN/GaN N2O BCl3
Page 24© Oxford Instruments 2018
Si etching
• Etch rate 2 to 7Å/cycle (up to 70Å/min)
• Cl2 used in dose step, Ar used for etch
• Anisotropic profile
ALE processing results
25nm wide Si
trenches etched to
110nm depth by
ALE, HSQ mask
still in place
MoS2 etching and Raman results
• Small shift in peaks per 3 ALE cycle
• 40 ALE cycles removed all material
• Starting thickness 18 nm
• Cl2 used in dose step, Ar used for etch
• Low damage with no defect induced
peak at 227 cm-1
Raman spectra
after 17, 20 and
23 ALE cycles
200 225 250 350 400 450 5000
50
100
150
200
17 Cycles
20 Cycles
23 Cycles
Inte
nsity (
a.u
.)
Raman Shift (cm-1)
Page 25© Oxford Instruments 2018
AlGaN/GaN ALE results: Ar/Cl2
• Etch rate 1.5-3 Å/cycle (up to 18 Å/min)
• Uniformity <±5% over 200mm
• Added roughness <<1nm. AFM data
indicates a smoothening effect
AFM data courtesy of Paolo Abrami in Collaboration with Bristol Uni
ALE smoothening
0
1
2
3
4
5
6
7
0 10 20 30 40
AlG
aN E
PC
(Å/c
ycle
)
DC bias (V)
with Cl2
No Cl2
AlGaN etching rate per cycle
(pm
)
AlGaN surface roughness decreases with ALE
Page 26© Oxford Instruments 2018
Atomic Scale Processing Cluster
Page 27© Oxford Instruments 2018
Conclusions
• ALD can be tuned to be low damage but ion energy can also be enhanced.
• Oxide film stress dependant on material (e.g. crystal phase) and plasma
conditions.
• Biasing allows low-resistivity nitrides and improved superconductive
properties. Novel plasma gases allows growth of fluorides and sulfides.
• Wide range of ALE processes available.
• ALE of silicon but also low damage etching of 2D materials such as MoS2.
• Smoothening of AlGaN observed. Could be important feature of ALE.
• Processes can be combined in cluster tool to allow atomic scale processing and
find synergy of alternating between processes and doing process flow in vacuum.