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Pietro P. Altermatt Trina Solar Changzhou, China
Solar cells made of crystalline silicon:
successful mainstream thanks to
intense research and development
Presentation at the Oxford Energy Network, Oxford University, GB 7. Nov. 2017
2 Altermatt, Trina Solar
A common solar module
module
cell
4 bus bars
front metal fingers
contains 60 cells
15.4 15.4 cm2
delivers about 300 Watts
3 Altermatt, Trina Solar
Photovoltaic (PV) principle
Two-level system
4 Altermatt, Trina Solar
Photovoltaic (PV) principle
1 Photo generation
Two-level system
5 Altermatt, Trina Solar
Photovoltaic (PV) principle
1
2
Photo generation
Transport
Two-level system
6 Altermatt, Trina Solar
Photovoltaic (PV) principle
1
2 3
4
Photo generation
Transport Contact External circuit
Two-level system
7 Altermatt, Trina Solar
Photovoltaic (PV) principle
1
2 3
4
5
Photo generation
Work
Transport Contact External circuit
Two-level system
8 Altermatt, Trina Solar
Photovoltaic (PV) principle
1
2 3
4
5
6 7
Photo generation
Work
Second contact
Transport Contact External circuit
Two-level system
9 Altermatt, Trina Solar
Photovoltaic (PV) principle
1
2 3
4
5
6 7
Photo generation
Work
Second contact
Transport Contact External circuit
Two-level system
10 Altermatt, Trina Solar
Photovoltaic (PV) principle
Two-level system
Metals not suitable (recombination)
Most solar cells are made of crystalline silicon (semiconductor)
11 Altermatt, Trina Solar
Photovoltaic (PV) principle
Two-level system
Metals not suitable (recombination)
12 Altermatt, Trina Solar
Photovoltaic (PV) principle
1 Photo generation
Metals not suitable (recombination)
Most insulators not suitable (insufficent absorption)
13 Altermatt, Trina Solar
Photovoltaic (PV) principle
1 Photo generation
Metals not suitable (recombination)
Most insulators not suitable (insufficent absorption)
Bands
14 Altermatt, Trina Solar
Photovoltaic (PV) principle
1
2
Photo generation
Transport
Two-level system
Metals not suitable (recombination)
Most insulators not suitable (insufficent absorption)
Thinner cells don’t need good transport
Silicon cell:
170 m thick
Si cell
15 Altermatt, Trina Solar
Photovoltaic (PV) principle
1
2 3
4
Photo generation
Transport Contact External circuit
Two-level system
Metals not suitable (recombination)
Most insulators not suitable (insufficent absorption)
Thin cells don’t need transport
Different carrier inside than outside possible
16 Altermatt, Trina Solar
Photovoltaic (PV) principle
1
2 3
4
5
Photo generation
Work
Transport Contact External circuit
Two-level system
Power = current voltage, (IV)
Metals not suitable (recombination)
Most insulators not suitable (insufficent absorption)
Thin cells don’t need transport
Different carrier inside than outside possible
Too small gap gives too small voltage
17 Altermatt, Trina Solar
Photovoltaic (PV) principle
1
2 3
4
5
Photo generation
Work
Transport Contact External circuit
Two-level system
Power = current voltage, (IV)
Metals not suitable (recombination)
Most insulators not suitable (insufficent absorption)
Thin cells don’t need transport
Different carrier inside than outside possible
Too small gap gives too small voltage
18 Altermatt, Trina Solar
Photovoltaic (PV) principle
1 2
3 4
5
Photo generation
Work
Transport Contact External circuit
Two-level system
Power = current voltage, (IV)
Metals not suitable (recombination)
Most insulators not suitable (insufficent absorption)
Thin cells don’t need transport
Different carrier inside than outside possible
Too small gap gives too small voltage
19 Altermatt, Trina Solar
Photovoltaic (PV) principle
1
2 3
4
5
6 7
Photo generation
Work
Second contact
Transport Contact
Two-level system
Homogeneous system: semiconductor is required, Si is a good choice
20 Altermatt, Trina Solar
Overview
1. Mainstream Si solar cell production
2. Improvements from research development production
3. Conditions for research ideas or new inventions to enter mainstream
21 Altermatt, Trina Solar
Overview
1. Mainstream Si solar cell production
2. Improvements from research development production
3. Conditions for research ideas or new inventions to enter mainstream
22 Altermatt, Trina Solar
From quartz sand to silicon?
1. High-purity quartz sand needed.
2. Production of metallurgical Si mostly for steel/Al/silicone industry
SiO2 + C → SiO(gas) + CO
SiO + CO → Si + CO2
Electrically heated furnace
about 1900C
with carbon arc
Si melts
at 1414C
23 Altermatt, Trina Solar
Silicon purified by distillation
1. High-purity quartz sand needed.
2. Production of metallurgical Si mostly for steel/Al industry
3. Small part of it is being purified:
distillation via SiHCl3 (trichlorosilane, TCS)
Si + 3 HCl → HCl3Si + H2
24 Altermatt, Trina Solar
Decomposition to solar grade silicon
1. High-purity quartz sand needed.
2. Production of metallurgical Si mostly for steel/Al industry
3. Distillation via SiHCl3
4. Pyrolytic decomposition (Siemens process) or fluidized-bed deposition
5. Solar grade silicon
REC, Norway
25 Altermatt, Trina Solar
Monocrystalline silicon
Czochralski pulling of monocrystalline ingots
(1 mm/minute) Courtesy: SolarWorld Courtesy: Fraunhofer CSP
26 Altermatt, Trina Solar
Multicrystalline silicon
Cast silicon via
direcitonal
solidification
15 mm/h
cut into bricks
15.4 cm
27 Altermatt, Trina Solar
Sawing into wafers
H. Lauvray et al,
New wire silicon slicing technology for solar cells,
3rd EU PV Conf. 1980, p. 603
Si ingot
wire
free abrasives, “slurry”
kerf loss
fixed abrasives
“diamond wire”
Multi-wire sawing
28 Altermatt, Trina Solar
PERC
8 main fabrication steps
29 Altermatt, Trina Solar
Saw damage etching, texturing
10 μm
A. Hauser et al, 19th EU PV Conf. 2004, p. 1094
30 µm
Courtesy: ISFH
KOH etch acidic etch
University of Constance
30 Altermatt, Trina Solar
Texturing
“old” days without acidic texturing
multi
mono
nowadays with acidic texturing
University of Constance
31 Altermatt, Trina Solar
Phosphorus diffusion
20 – 30 min, 750C
Courtesy: Centrotherm
p-type wafer
J. Mandelkorn et al., J El Chem Soc 109, 313 (1962)
n-type
(conductive
for electrons)
cross-section
of cell
32 Altermatt, Trina Solar
Rear side etching
Courtesy: Schmid
Emitter
33 Altermatt, Trina Solar
Emitter etch back
H. Haverkamp et al., 33rd IEEE PV Conf (2008), no 112
University of
Constance
Emitter
34 Altermatt, Trina Solar
Front dielectric layer deposition
Palsma-enhanced chemical vapor deposition (PE-CVD)
SiH4 + NH3 + N2 SiNx + H2
Silane Silicon nitride
SiNx
35 Altermatt, Trina Solar
Front passivation and ARC
ISFH,
University of Hanover
90’s
Photo generation Passivation
SiNx
Si surface
similar to metal
36 Altermatt, Trina Solar
Front passivation and ARC
Courtesy: Meyer Burger
SiNx
37 Altermatt, Trina Solar
Rear passivation with Al2O3
Al2O3
SiNx
stack
University of Eindhoven 2006
University of Erlangen
B. Hoex et al, Appl Phys Lett 89, 042112 (2006)
38 Altermatt, Trina Solar
Rear passivation with Al2O3
Al2O3
SiNx
stack
University of Eindhoven 2006
University of Erlangen
Courtesy: Meyer Burger
39 Altermatt, Trina Solar
Rear laser opening
R. Preu et al., 16th EU PV Conf. (2000) 1181
ISE Freiburg
Courtesy: ISE
40 Altermatt, Trina Solar
Screen-printing of metal contacts
Paste
Screen
Squeegee
cell
Front silver fingers
Rear Al with Ag soldering pads
E.L. Ralph, 11th IEEE PV Specialists Conf. (1975), p. 315
Courtesy of www.gwent.org
Spectrolab (startup company)
41 Altermatt, Trina Solar
Screen-printing of metal contacts
< 100 mg silver/cell
42 Altermatt, Trina Solar
Firing-through ARC
IMEC, 1997
University of Constance, 2000 -> mass production
Conveyor belt furnace
Firing
2-3 seconds
800C
43 Altermatt, Trina Solar
Firing: Al back surface field
Firing
2-3 seconds
800C
electron conduction
hole conduction
emitter
back surface field (BSF)
44 Altermatt, Trina Solar
PERC
8 main fabrication steps
45 Altermatt, Trina Solar
Module and systems
46 Altermatt, Trina Solar
Overview
1. Mainstream Si solar cell production
2. Improvements from research development production
3. Conditions for research ideas or new inventions to enter mainstream
47 Altermatt, Trina Solar
Experience curve
48 Altermatt, Trina Solar
Experience curve
49 Altermatt, Trina Solar
Silicon shortage 2003 – 2012
30
20
10
0
19
95
20
00
20
05
20
10
kt
by-products of electronic industry
solar grade silicon
demand
Andrews and Clarson, Silicon 7, 303 (2015)
R&D on a multitude of more direct
purification/crystallization methods
M. Heuer, Semic & Semimet 89, 77 (2013)
50 Altermatt, Trina Solar
Only established methods survived in oversupply
R. Fu etal., IEEE J PV 5, 515 (2015)
Today:
electronic industry: 30 000 t
solar industry: 460 000 t
US$ 15/kg (spot price)
Siemens processes
Fluidized bed
Reality in 2013,
in oversupply
51 Altermatt, Trina Solar
Established methods get optimized
Yadav et al., Ren & Sust En Rev 78, 1288 (2017)
Siemens process
(pyrolytic decompostion of e.g. SiHCl3)
Hard to compete against
optimized standard
52 Altermatt, Trina Solar
Over- and under-supply
Fast growing industries go through
cycles of under and over-supply
In times of over-supply,
many ideas die
Glo
bal annual P
V p
roduction
[GW
]
Year
53 Altermatt, Trina Solar
Experience curve: different interpretations
54 Altermatt, Trina Solar
Production shifted to China
Mark
et
share
Year
China
US
Japan
Germany Taiwan
Malaysia Thailand
Vietnam
2017
55 Altermatt, Trina Solar
Production shifted to China
Mark
et
share
Year
China Japan
Taiwan
Malaysia Thailand
Vietnam
2017
Antidumping duties: 27.3% – 64.9%
Added anti-subsidy duties: 11.5%
Combined duties should not be higher than
76.4% in future
EU Commission
Sept. 2017:
courtesy: Wikipedia
US
Germany
56 Altermatt, Trina Solar
Innovation or economy of scale?
C. Zheng. D.M.Kammen, Energy Policy 67, 159 (2014)
57 Altermatt, Trina Solar
Recent innovations
• Fluidized-bed deposition of Si (REC, Norway)
• Acidic texturization of multi Si (University Constance)
• Rear Al2O3 passivation (University of Eindhoven)
• Rear etching (mainly German tool companies)
• Rear laser ablation (ISE Freiburg)
• High-performance multi (National Taiwan University)
• Diamond wire sawing (companies in Japan and Taiwan)
• Texturing of diamond-wire sawn mutli wafers (start-ups in China)
• Improvements of screen-printing pastes (global paste companies)
Most recently:
Already mentioned:
58 Altermatt, Trina Solar
Recent innovations
• Fluidized-bed deposition of Si (REC, Norway)
• Acidic texturization of multi Si (University Constance)
• Rear Al2O3 passivation (University of Eindhoven)
• Rear etching (mainly German tool companies)
• Rear laser ablation (ISE Freiburg)
• High-performance multi (National Taiwan University)
• Diamond wire sawing (companies in Japan and Taiwan)
• Texturing of diamond-wire sawn mutli wafers (start-ups in China)
• Improvements of screen-printing pastes (global paste companies)
Most recently:
Already mentioned:
European grant bodies often do not want
Chinese companies being involved
in a grant application
Buying and installing Chinese solar modules in the EU:
70% of revenue generated within EU, only 30% in China.
59 Altermatt, Trina Solar
Contact difficult to understand and manipulate
metal
conduction
tunneling
through
glass layer
Ag colloid-assisted
tunneling
H. Mäckel, P.P. Altermatt, IEEE J. of PV 5, 1034 (2015)
Fastest improvements
during over-supply
Silicon Silicon
60 Altermatt, Trina Solar
Innovation or economy of scale?
Yearly staff turnover in China: 60% in production, 40% in R&D (pollination)
61 Altermatt, Trina Solar
Factory doubles every 2½ years
62 Altermatt, Trina Solar
Factory doubles every 2½ years
63 Altermatt, Trina Solar
Overview
1. Mainstream Si solar cell production
2. Improvements from research development production
3. Conditions for research ideas or new inventions to enter mainstream
64 Altermatt, Trina Solar
Fabrication requirements
• Annual production of modules surpasses 100 GW.
• Silver used per cell is below 100 mg; still, PV industry is main silver consumer.
• Cells are produced in a one-second sequence, so each fabrication step must
not take longer than one second (e.g. P diffusion for 20 min on 1200 wafers)
• Warranty for modules given for 20 – 30 years.
Until then, the module power must decrease only by a very few percent.
• The energy pay-back time is about one year (including Si and Ag production).
• A Si wafer costs 40 pence (spot-price); fabrication costs 25 pence per cell;
60 cells in module makes 40 pounds; module fabrication cost 25 pounds.
Costs are falling 18% per year
Hence, improvement or alternatives must:
• grow to large output,
• be stable over 20 – 30 years,
• must not consume scarce materials or lots of energy,
• must be fabricated fast,
• and be cheap and cheaper.
65 Altermatt, Trina Solar
Suggestions from previous slides
Entering mainstream solar cell production:
• Good collaboration between university and tool manufacturers
• Don’t keep your invention secret, you will stay alone
• Don’t grant an exclusive license of your patent, they will stay alone
• Stimulate a whole community to develop your invention to production
66 Altermatt, Trina Solar
Experience curve for CdTe and CIGS
Y. Chen, Feng, Verlinden, 6th World Conf PV, 2014, paper 9WeO.5.5
CIGS
too flat
67 Altermatt, Trina Solar
Where is mainstream heading to?
Colors:
various existing technologies
continuously being
developed further
B. Min, H. Wagner, M. Müller, H. Neuhaus, R. Brendel, P.P. Altermatt, 31st EU PV Conf. 2015 p. 473.
Device
modeling
PERC cells
68 Altermatt, Trina Solar
Cells are getting more efficient
PERC cell efficiency
is expected to increase
by about 0.4%abs each year
Y. Chen, Feng, Verlinden, 6th World Conf PV, 2014, paper 9WeO.5.5
69 Altermatt, Trina Solar
Better and cheaper mainstream cells
In about 8 years* PERC cells may come close to 23% – 24% cell efficiency,
but require every 2 years a new technological step
while module cost may go down to about half.
* if no major disruption or breakthroughs
P.P. Altermatt et al, 44th IEEE PV Conf. Wasington, July 2017
Currently: module fabrication cost 65 pounds
70 Altermatt, Trina Solar
New PV material into mainstream?
Cell efficiency can be improved further
e.g. by adding an other layer of PV material
on top of PERC cells (hetero-emitter),
and/or by introducing passivated contacts
electron conduction
hole conduction
hetero emitter
(other than Si)
passivated contact
A. Louwen, Sol En Mat & Sol Cells 147,295 (2016)
71 Altermatt, Trina Solar
Current research topics
Current research topics in silicon PV (cells, not modules):
• Passivated contacts
• n-type Si material
• Replacement of Al2O3 passivation
• Narrower front metal fingers
• Hetero-emitter (organic material?)
• Tandem cells
72 Altermatt, Trina Solar
Categories of PV
1st generation
2nd generation
3rd generation
Standard silicon solar cells (e.g. PERC)
Thin-film cells (e.g. CdTe, other semiconductors)
Quantum-engineered material
(e.g. quantum dots, hetero-structures, perovskites)
M. Green, Prog in PV 9, 123 (2001)
73 Altermatt, Trina Solar
Categories of PV
M. Green, Prog in PV 9, 123 (2001)
May cells, made of
other material than Si,
replace Si cells?
74 Altermatt, Trina Solar
30% or 40% efficient cells?
Calculations: ISE Freiburg
If cell efficiency is lifted to
30% (or 40%) the cell
must cost only maximally
55% (70%) more to be
competitive.
Crucial consequences for basic research
to have a prospect
for being applied one day
75 Altermatt, Trina Solar
30% or 40% efficient cells?
?
76 Altermatt, Trina Solar
Mainstream PV is important for climate
2C
3C
3.5C
>4C
Paris:
increased
ambition
Paris:
continued
ambition
Low policy
No policy
Research & development which benefits mainstream silicon PV
has a direct and significant impact on climate
global warming:
www.trinasolar.com
78 Altermatt, Trina Solar
Forecast in 2016
79 Altermatt, Trina Solar
Forecast in 2016
80 Altermatt, Trina Solar
Silver forecast
C. Muschelknautz, 4th Metallization Workshop, Constance, 2013
81 Altermatt, Trina Solar
Silver forecast
C. Muschelknautz, 4th Metallization Workshop, Constance, 2013
82 Altermatt, Trina Solar
Silver forecast
C. Muschelknautz, 4th Metallization Workshop, Constance, 2013
83 Altermatt, Trina Solar
Early, forgotten work in Manchester
A.D. Haigh, 12th IEEE PV Conf (1976), 360
Ferranti Ltd, Manchester
84 Altermatt, Trina Solar
Where is R&D done?
Tool manufacturers vs. PV companies
GCL
LONGi
85 Altermatt, Trina Solar
Passivated contacts
Sentaurus simulation
Highly-doped silicon behind oxide enables:
minority tunneling hindered
(large ox barrier) and/or depletion
majority band edge lower behind
oxide than at the front of the oxide
Conditions:
minority carrier depletion at the Si/SiO2
interface to reduce recombination
(passivation)
majority carrier accumulation
to enhance tunneling
passivated majority contact
directly on lowly doped n-type base
SiO2
pc-Si c-Si
n-type
1 Ωcm
n-type
highly-
doped
MPP (600 mV)
86 Altermatt, Trina Solar
Materials for passivated contacts
defect band
MoOx
Metal
Bullock et al, Appl Phys Lett 105, 232109 (2014)
Oxide layer can be made thicker
if there is a defect band
87 Altermatt, Trina Solar
Solar cell materials for global mass production
CdTe, CIGS
1980 – 1998: 2008 Navigant Consulting report; 1999-2009: March issues of Photon International; 2010-2015: IHS 2015 Q4 market
report.
88 Altermatt, Trina Solar
Where is mainstream heading to?
Colors:
various existing technologies
continuously being
developed further
B. Min, H. Wagner, M. Müller, H. Neuhaus, R. Brendel, P.P. Altermatt, 31st EU PV Conf. 2015 p. 473.
Device
modeling
PERC cells
Introduce these technologies
at a suitable
development stage
ineffective
effective
89 Altermatt, Trina Solar
Transition from standard to PERC cell
standard cell PERC cell
Global production capacity of Si cells (GW)
PERC
standard
Expected from orders at tool manufactures Forecast
90 Altermatt, Trina Solar
Price decay for roadmap (linear plot over time)