Atomic Layer Deposition Atomic Layer Deposition (ALD) Erwin - - PowerPoint PPT Presentation
Atomic Layer Deposition Atomic Layer Deposition (ALD) Erwin - - PowerPoint PPT Presentation
Atomic Layer Deposition Atomic Layer Deposition (ALD) Erwin Kessels w.m.m.kessels@tue.nl www.phys.tue.nl/pmp Vapor phase deposition technologies Physical Vapor Deposition (PVD) Chemical Vapor Deposition (CVD) sputtering Heat!
Vapor phase deposition technologies
Physical Vapor Deposition (PVD) – sputtering – Chemical Vapor Deposition (CVD)
Energetic ions! Heat!
/Applied Physics - Erwin Kessels
g
More applications have stricter requirements on
1. Precise growth and thickness control 2 Hi h f lit / t 2. High conformality/step coverage 3. Good uniformity on large substrates 4. Low substrate temperatures
/Applied Physics - Erwin Kessels
Very demanding applications
Nanoelectronics Photovoltaics f Protective thin films Flexible electronics
/Applied Physics - Erwin Kessels
CMOS scaling in nanoelectronics
??? ??? graphene graphene
Active Area Gate Field Spacers Active Area Gate Field Spacers Active Area Gate Field Spacers??? ??? ??? ???
Active Area Gate Field Spacers Active Area Gate Field Spacers Active Area Gate Field SpacersGe/IIIV Ge/IIIV nanowires nanowires g p g p
HfO
metal gate metal gate FinFET FinFET
L=35nm
SiGe
L=35nm L=35nm
SiGe
strain strain
HfO 2
high high -
-
time
silicide silicide USJ USJ
Time
Courtesy of Marc Heyns, IMEC
/Applied Physics - Erwin Kessels
Field-effect transistor: replacing SiO2 by HfO2
32 nm Thermally grown SiO2 Thermally grown SiO2
/Applied Physics - Erwin Kessels
Precise deposition of nanometer-thick Hf-based oxides
www.chipworks .com
Field-effect transistor: going from 2D to 3D gates
22 nm Precise deposition of nanometer-thick Hf-based oxides with excellent conformality
/Applied Physics - Erwin Kessels
with excellent conformality
www.chipworks .com
Outline
1. Atomic layer deposition (ALD): basics and key features 2. ALD equipment 3. Materials & ALD surface chemistries 4. Some applications of ALD 5. Recent developments in high-throughput ALD
/Applied Physics - Erwin Kessels
Atomic Layer Deposition (ALD)
- Reactants (precursors) are pulsed into reactor alternately and cycle-wise (ABAB..)
- Precursors react through saturative (self-limiting) surface reactions
- A sub-monolayer of material deposited per cycle
/Applied Physics - Erwin Kessels
ALD of Al2O3 films: Al(CH 3)3 - H 2O process
/Applied Physics - Erwin Kessels
Thickness vs. number of cycles
Film thickness is ruled by the number of cycles chosen 30
- 1. Al(CH3)3
2 S
iH {N(C H )}
H3C Al CH3 CH3 N(C2H5)2
30
1. Al2O3 2. SiO2 3. Ta2O5
m)
- 2. S
iH2{N(C2H5)}2 3 T {N(CH ) }
N(CH3)2 Si H H N(C2H5)2
20
2 5
4. ZnO2 5. TiO2
ness (nm
- 3. Ta{N(CH3)2}5
(H3C)2N Ta N(CH3)2 N(CH3)2 (
3)2
N(CH3)2
10
Thickn
- 4. Zn(CH2CH3)2
H3C H2 C Zn H2 C CH3
50 100 150 200 250
ALD C l
- 5. Ti(Cp*)(OCH3)3
Ti H3CO OC OCH3 H3C CH3 CH3 H3C CH3
+
/Applied Physics - Erwin Kessels
Potts et al., J. Electrochem. Soc., 157, P66 ( 2010). Dingemans et al., J. Electrochem. Soc. 159, H277 (2012)
ALD Cycles
H3CO OCH3
+
H2O, O3, or O2 plasma
Key features of ALD
1. Control of film growth and thickness ‘Digital’ thickness control 2. High conformality/step coverage Self-limiting surface reactions 3 G d if it l b t t 3. Good uniformity on large substrates 300 mm and even bigger 4. Low substrate temperatures p Between 25 - 400 °C 5. Multilayer structures and nanolaminates Easy to alternate between processes 6. Large set of materials and processes Many different materials demonstrated Many different materials demonstrated
/Applied Physics - Erwin Kessels
Line-of-sight vs. conformal grow th
/Applied Physics - Erwin Kessels
Materials deposited ALD
/Applied Physics - Erwin Kessels
Puurunen, J. Appl. Phys. 97, 121301 (2005) Miikkulainen et al., J. Appl. Phys. 113, 021301 (2013).
Outline
1. Atomic layer deposition (ALD): basics and key features 2. ALD equipment 3. Materials & ALD surface chemistries 4. Some applications of ALD 5. Recent developments in high-throughput ALD
/Applied Physics - Erwin Kessels
Single w afer ALD reactor
Shower head reactor (warm or hot wall reactor) Flow-type reactor (hot wall reactor)
- Temporal ALD
P l t i f
- Pulse-train of precursors
- Reactor pressure 1-10 Torr
- Applications: semiconductor (logic)
/Applied Physics - Erwin Kessels
pp ( g )
Batch ALD reactor
Temporal ALD
Batch reactor
- Temporal ALD
- Typically 50-500 substrates in a single deposition run
- Single-side deposition can be challenging
g p g g
- Applications: semiconductor (memory), displays,
solar cells, etc.
/Applied Physics - Erwin Kessels
Plasma ALD reactors
Plasma-assisted ALD can yield additional benefits for specific applications: 1. Improved material properties 2. Deposition at lower temperatures (also room temperature) Direct plasma Remote plasma p p ( p ) 3. Higher growth rates/cycle and shorter cycle times 4. More versatility/freedom in process and materials etc. Direct plasma Substrate part of plasma creation zone Remote plasma Substrate “downstream” of plasma creation zone
/Applied Physics - Erwin Kessels
Heil et al., J. Vac. Sci. Technol. A 25, 1357 (2007). Profijt et al., J. Vac. Sci. Technol. A 29 050801 (2011)
Plasma-based chemistry (metal oxides)
1. Al(CH3)3
2.
H3C Al CH3 CH3 Si N(C2H5)2
2 0
Al2O3 TiO2 - Ti(O
iPr)4
e)
SiH2{N(C2H5)}2 3. Ta{N(CH3)2}5
(H3C)2N Ta (C ) N(CH3)2 N(CH3)2 Si H H N(C2H5)2
1.6 2.0
2 3 2
( )4 SiO2 TiO2 - Ti(Cp
Me)(O iPr)3
Ta2O5 TiO2 - Ti(Cp*)(OMe)3
e (Å/cycle
(
3)2 5
4. Ti(OiPr)4
N(CH3)2 N(CH3)2 Ti
i
OiPr
0.8 1.2
per Cycle
4
5. Ti(CpMe)(OiPr)3
Ti Ti
iPrO
OiPr OiPr CH3
0 0 0.4
Growth
3
6. Ti(Cp*)(OCH )
Ti
iPrO
OiPr OiPr H3C CH3 CH3
50 100 150 200 250 300 0.0
Substrate Temperature (°C)
/Applied Physics - Erwin Kessels
Ti(Cp*)(OCH3)3
Ti H3CO OCH3 OCH3 H3C CH3
Potts et al., J. Electrochem. Soc., 157, P66 ( 2010). Dingemans et al., J. Electrochem. Soc. 159, H277 (2012)
Oxford Instruments OpAL reactor – Plasma ALD
/Applied Physics - Erwin Kessels
ALD equipment suppliers (incomplete list)
Semiconductor Solar / R2R R& D / Pilot
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Outline
1. Atomic layer deposition (ALD): basics and key features 2. ALD equipment 3. Materials & ALD surface chemistries 4. Some applications of ALD 5. Recent developments in high-throughput ALD
/Applied Physics - Erwin Kessels
Metalorganic and H 2O: ligand exchange (Al2O3)
Al(CH3)3 exposure Purge
10
- 8
H O ry signal (A)
Al(CH3)3 Al(CH3)3 Al(CH3)3 Al(CH3)3 H2O H2O H2O H2O
10
- 8
H O ry signal (A)
10
- 8
H O ry signal (A)
Al(CH3)3 Al(CH3)3 Al(CH3)3 Al(CH3)3 H2O H2O H2O H2O
10
- 10
10
- 9
H2O spectrometr CH4
10
- 10
10
- 9
H2O spectrometr CH4
10
- 10
10
- 9
H2O spectrometr CH4
AlOH*+ Al(CH3)3 AlOAl(CH3)2* + CH4
Cycle
25 50 75 100 10
- 11
Mass Time (s)
4
25 50 75 100 10
- 11
Mass Time (s)
4
25 50 75 100 10
- 11
Mass Time (s)
4
AlOH Al(CH3)3 AlOAl(CH3)2 CH4
Surface chemistry rules ALD process: ligand exchange between Al(CH ) and
AlOH* + CH4 AlCH3* + H2O
ligand exchange between Al(CH3)3 and –OH surface groups and H2O and –CH3 surface groups leads to CH4 reaction products
* are surface species
H2O exposure Purge
/Applied Physics - Erwin Kessels
Metalorganic and H 2O: ligand exchange (Al2O3)
Al(CH3)3 exposure Purge
10
- 8
H O ry signal (A)
Al(CH3)3 Al(CH3)3 Al(CH3)3 Al(CH3)3 H2O H2O H2O H2O
10
- 8
H O ry signal (A)
10
- 8
H O ry signal (A)
Al(CH3)3 Al(CH3)3 Al(CH3)3 Al(CH3)3 H2O H2O H2O H2O
10
- 10
10
- 9
H2O spectrometr CH4
10
- 10
10
- 9
H2O spectrometr CH4
10
- 10
10
- 9
H2O spectrometr CH4
Cycle
25 50 75 100 10
- 11
Mass Time (s)
4
25 50 75 100 10
- 11
Mass Time (s)
4
25 50 75 100 10
- 11
Mass Time (s)
4
Surface chemistry rules ALD process: ligand exchange between Al(CH ) and ligand exchange between Al(CH3)3 and –OH surface groups and H2O and –CH3 surface groups leads to CH4 reaction products
H2O exposure Purge
/Applied Physics - Erwin Kessels
Metalorganic and H 2O: ligand exchange (Al2O3)
4x10
- 5
rbance
2940 cm-1 1207 cm-1
Al(CH3)3 chemisorption
Al(CH3)3 exposure Purge frared abso
OH stretching CHx stretching CHx deformation 2940 cm 1 1207 cm 1
H O
4000 3500 3000 2500 2000 1500 1000
In Wavenumber (cm
- 1)
H2O exposure
Cycle
Surface chemistry rules ALD process: Surface alternately covered by –OH Surface alternately covered by –OH surface groups and –CH3 surface groups
/Applied Physics - Erwin Kessels
H2O exposure Purge
Metalorganic and H 2O: ligand exchange (Al2O3)
0.8 1.2
Cycle (Å)
Al(CH3)3 exposure Purge
0.4
- wth per C
20 40 60 0.0
Gro Al(CH3)3 dose (ms)
Cycle
Conditions such that precursors react through saturative surface reactions: Al(CH3)3 does not react with –CH3 surface groups
/Applied Physics - Erwin Kessels
H2O exposure Purge
Metalorganic and H 2O: ligand exchange (Al2O3)
0 8 1.2
ycle (Å)
Al(CH3)3 exposure Purge
0.4 0.8
wth per Cy
20 40 60 80 0.0
Grow H2O dose (ms) Cycle
Conditions such that precursors react through saturative surface reactions: H2O does not react with –OH surface groups
/Applied Physics - Erwin Kessels
H2O exposure Purge
Metalorganic and H 2O: ligand exchange (Al2O3)
1.2 1.6
cle (Å)
Al(CH3)3 exposure Purge
0.4 0.8
wth per Cyc
CVD+ALD ALD 2 4 6 8 0.0
Grow Purge after Al(CH3)3 dose (s) Cycle
Precursors and reactants should be very well evacuated/separated from reactor before pulsing the next precursor/reaction: Otherwise parasitic CVD
/Applied Physics - Erwin Kessels
H2O exposure Purge
ALD process: saturation curves (Al2O3)
(a)
0.15 0.20
(nm/cycle)
Thermal ALD - Al(CH3)3 & H2O
0.05 0.10
wth per Cycle (
CVD
Subsaturation
CVD
0 20
le)
(b)
20 40 60 80 100
0.00
Grow
Dose time (ms)
1 2 3 4 5
Purge time (s)
20 40 60 80
H2O dose (ms)
1 2 3
Purge time (s)
Plasma ALD - Al(CH3)3 & O2 plasma
0.10 0.15 0.20
Cycle (nm/cycl Subsaturation
20 40 60 80 100
0.00 0.05
Growth per C
1 2 3 4 5 1 2 3 4 5 1 2 3
CVD
/Applied Physics - Erwin Kessels
Dose time (ms) Purge time (s) Plasma time (s) Purge time (s)
ALD process: substrate temperature (Al2O3)
e)
0.2
Plasma ALD Thermal ALD e (nm/cycle
(a) 0.0 0.1
Growth rate
3 4 5 6 (b)
per cycle cm
- 2)
1 2 3
# Al atoms (10
15 c
100 200 300 400
Substrate temperature (
- C)
AlOH* + Al(CH3)3 AlOAl(CH3)2* + CH4
/Applied Physics - Erwin Kessels
(
3)3
(
3)2 4
AlOH* + CH4 AlCH3* + H2O
Van Hemmen et al., J. Electrochem. Soc. 154, G165 (2007) Potts et al., J. Electrochem. Soc., 157, P66 ( 2010).
ALD process: substrate temperature (ideal case)
ALD Temperature Window
- A. Condensation
B Insufficient
Window
Cycle
A C A C
- B. Insufficient
thermal energy
- C. CVD
wth per C
B
- D. Evaporation
H2O
Grow
B D B D
OH OH O ∆T
Substrate Temperature
Substrate/film surface
/Applied Physics - Erwin Kessels
Metal halide: ligand exchange (HfO2 and TiN)
HfOH* + HfCl HfOHfCl * + HCl Metal oxides: ligand exchange HfOH* + HfCl4 HfOHfCl3* + HCl HfOH* + HCl HfCl* + H2O TiNH* + TiCl TiNTiCl * + HCl Metals nitrides: ligand exchange TiNH + TiCl4 TiNTiCl3 + HCl TiNH2* + HCl TiCl* + NH3
/Applied Physics - Erwin Kessels
* are surface species
Metals: combustion (Pt) and reduction (W)
Noble metals: combustion by chemisorbed O2 3 O* + 2 (MeCp)PtMe3 2 (MeCp)PtMe2* + CH4 + CO2 + H2O 2 Pt* + 3 O* + 16 CO2 + 13 H2O 2 (MeCp)PtMe2* + 24 O2
Pt
Metals: fluorosilane elimination reactions WSiF H* + WF WWF * + SiF H WSiF2H + WF6 WWF5 + SiF3H WSiF2H* + SiF3H + 2H2 WWF5* + Si2H6
/Applied Physics - Erwin Kessels
* are surface species
Plasma-based chemistry (Al2O3 and TiN)
Metal oxides: combustion AlOH*+ Al(CH3)3 AlOAl(CH3)2* + CH4 AlOH* + CO2 + H2O AlCH3* + 4O Metal nitrides: ligand exchange and reduction TiNH* + TiCl TiNTiCl * + HCl TiNH + TiCl4 TiNTiCl3 + HCl TiNH2* + HCl TiCl* + 3H + N
/Applied Physics - Erwin Kessels
* are surface species
ALD of doped films, ternary compounds, etc.
/Applied Physics - Erwin Kessels
ALD of Al-doped ZnO films
Zn(C2H5)2 + H2O ZnO + 2 C2H6 ZnO ZnO:Al
n cycles ZnO + m cycles Al2O3
10
1
150 ºC Al2O3 TMA or DMAI + H2O
10 TMA
cm)
2
10
- 1
sistivity (
5 10 15 20 25 30 10
- 3
10
- 2
Res
DMAI
/Applied Physics - Erwin Kessels
Wu et al., J. Appl. Phys. 114, 024308 (2013)
5 10 15 20 25 30
Al fraction (at.%)
Outline
1. Atomic layer deposition (ALD): basics and key features 2. ALD equipment 3. Materials & ALD surface chemistries 4. Some applications of ALD 5. Recent developments in high-throughput ALD
/Applied Physics - Erwin Kessels
Thin-film electroluminescent (TFEL) displays
New large-area display in 1983
Atomic layer deposited ZnS:Mn 1974 First patent on ALD filed by Tuomo Suntala 1983 Introduction of first ALD (non)-transparent inorganic TFEL display Since 1989 Commercial production of ALD-TFEL displays by Planar
/Applied Physics - Erwin Kessels
- T. Suntola, Mater. Sci. Rep. 4, 261 (1989)
Encapsulation of OLED Devices
No encapsulation Thin-film-encapsulated OLEDs after testing 40 nm ALD Al2O3 film
Thin film encapsulation requires:
- low deposition temperatures
- low water vapor transmission rates
- low pinhole (black spot) density
/Applied Physics - Erwin Kessels
Langereis et al., Appl. Phys. Lett. 89, 081915 (2006). Keuning et al., J. Vac. Sci. Technol. A 30, 01A131 (2012).
Defect (dust particle) encapsulation
/Applied Physics - Erwin Kessels Courtesy of Jian Jim Wang (NanoNuvo Corporation, US A)
ALD films for photovoltaics
CIGS solar cells Dye-sensitized solar cells c-Si solar cells Organic solar cells Buffer layers Zn(O S ) Barrier layer Al O HfO Surface passivation Transparent conductive oxide On the verge of Zn(O,S ) (Zn,Mg)O In2O3 l Al2O3, HfO2, TiO2, etc. Photoanode Z O S O p Al2O3 ZnO:Al Electron selective layer industrial application High-throughput equipment Encapsulation Al2O3 ZnO, S nO2, TiO2, etc. Blocking layer Encapsulation Al2O3, ZnO, TiO2 selective layer
/Applied Physics - Erwin Kessels
Van Delft et al., S
- emicond. S
- ci. Technol. 27, 074002 (2012).
q p available g y HfO2, S nO2, TiO2 p Al2O3
Outline
1. Atomic layer deposition (ALD): basics and key features 2. ALD equipment 3. Materials & ALD surface chemistries 4. Some applications of ALD 5. Recent developments in high-throughput ALD
/Applied Physics - Erwin Kessels
Large substrate ALD reactors
- Temporal ALD
- Can be (inline) single wafer or batch reactor
- Substrate size up to 120 x 120 cm2
- Applications: Thin-film transistors, encapsulation,
CIGS solar cells, transparent conductive oxides
b w w w .beneq.com
/Applied Physics - Erwin Kessels
Batch ALD reactor
- Temporal ALD
- Typically 50-500 substrates in a single deposition run
- Single-side deposition can be challenging
- Applications: semiconductor (memory), displays,
Applications: semiconductor (memory), displays, solar cells, etc.
/Applied Physics - Erwin Kessels
w w w .asm.com w w w .beneq.com
Spatial ALD concept
- Precursor and reactant pulsing occur at different positions
- The substrate or the “ALD deposition head” must move
The substrate or the ALD deposition head must move
- Purge areas created by inert gas barriers prevent CVD reactions
requires operation at high pressure
- No gas switching or vacuum pumps no deposition on the reactor walls
- No gas switching or vacuum pumps, no deposition on the reactor walls
/Applied Physics - Erwin Kessels
Spatial ALD: S2S and R2R
- Sheet-to-sheet (S2S, or wafer-to-wafer)
M i 1
w w w .levitech.nl
Movie 1 Movie 2
- Roll-to-roll (R2R)
w w w .solaytec.com
Movie 2
w w w .lotusat.com w w w .beneq.com w w w .tno.nl
Movie 3
/Applied Physics - Erwin Kessels
Summary
1. ALD can fulfill stricter requirements on thin film growth in terms of growth control, conformality, uniformity and low temperature 2 ALD is therefore complementary to PVD and CVD techniques 2. ALD is therefore complementary to PVD and CVD techniques 3. ALD relies on surface chemistry – not all materials can be prepared 4. ALD cycle yields sub-monolayer of film (typically 0.5 – 1 Å/ cycle) ( ) 5. ALD is gaining popularity also outside semiconductor industry 6. Runner up (method): Plasma ALD 7. Runner up (application): ALD for photovoltaics 8. High-volume manufacturing equipment is available 9 Equipment for batch ALD and S2S and R2R spatial ALD launched 9. Equipment for batch ALD and S2S and R2R spatial ALD launched
- 10. ALD has a bright future
/Applied Physics - Erwin Kessels
Further reading and dow nloads
Recent literature on ALD
- Book on ALD, Pinna and Knez (Eds.) Wiley VHC (2011)
, ( ) y ( )
- Kessels and Putkonen, MRS Bull. 36, 907 (2011)
Recent literature on plasma ALD p
- Profijt et al., J. Vac. Sci. Technol. A 29 050801 (2011)
Recent literature on ALD for PV Recent literature on ALD for PV
- Van Delft et al., Semicond. Sci. Technol. 27 074002 (2012)
- Bakke et al., Nanoscale 3, 3482 (2011)
/Applied Physics - Erwin Kessels
Title
/Department of Applied Physics