State of the art of amorphous Si thin film solar cells

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Universidade do Minho
Thin film silicon solar cells
and modules
Pedro Alpuim
Department of Physics
Universidade do Minho
Guimarães, Portugal
Mikkeli, March 17
17-19,
19, 2010, Finland
Outline
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•
•
•
Motivation: market analysis
a-Si:H
a
Si:H and nc-Si:H
nc Si:H thin film solar cell fundamentals
High efficiency concepts:
– Multijunction solar cells
– Light trapping
•
•
Low cost flexible thin film Si solar cells and modules
Conclusions
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Motivation: PV will continue to grow
US, Italy, and China, together 50% of the 2010 growth picture
Average Selling Prices
50
40
25
-25%
20
15
30
10
20
5
10
0
0
* * * *
Sources: iSupply, EPIA, DisplaySearch
Annual P
A
PV marrket (GW
Wp)
30
1998
1999
2000
2
2001
2
2002
2
2003
2
2004
2
2005
2
2006
2
2007
2
2008
2
2009
2
2010
2
2011
2
2012
2
2013
2
G
Global
ccumulattive PV
V
power in
p
nstalled
d (GWp)
60
Year
*estimated
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Motivation: thin film will grow
faster than wafer PV market
Source: OerlikonSolar, Photovoltaics World
2010-2012
2010• 2010 year of adapting FIT in Germany (others will follow…)
• Supply & demand will continue to swing between over and under supply
• Production capacity still exceeds installations (slower price decline than 2009)
• Margins reduced to installations, module prices under pressure
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Thin film PV: 3 leading technologies
Module production 2009: thin films => 496 MW; wafer => 1007 MW
Module prognostics 2010: thin films => 819 MW; wafer => 1658 MW
PV Modules (MWp)
1000
1000
production
d i 2009
capacity 2009
808
800
prognostic 2010
capacity 2010
988
800
Nano solar (640 MW)
600
600
318
400
200
FirstSolar (99%)
213 237
198
85
0
a-Si:H
Si H
CIGS
CdT
CdTe
400
367
428
225
227 237
200
0
a-Si:H
CIGS
CdTe
Thin film solar module production in Germany 2009
2009-2010
2010
Source: Photon
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Light absorption by thin
thin--film
materials for solar cells
A. Shah et. al., Thin Solid Films 502 (2006) 292
The efficiency of the solar cell
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•
The electric current in the PV cell depends on:
i) N
Number
b off electron-hole
l
h l pairs
i generated
db
by iincident
id
lilight
h
(absorption in the semiconductor)
ii) Carrier collection efficiency at the contacts (mobility-lifetime
product).
product)
•
•
•
The voltage depends on:
i) the
th b
bandgap
d
off th
the semiconductor
i
d t
ii) the doping level of the contacts
The fill factor depends on:
i) the series and the shunt resistances
ii)) the defect density
y in the i-layer
y
Operative electrical parameters of the solar cell are obtained from its
I – V curve.
The single junction aa-Si:H p
p--i-n solar cell
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Substrate
Superstrate
ZnO:Al SnO2:F
ZnO:Al,
p
Glass or transparent plastic
ZnO:Al, ZnO:Ga
p
TCO (0.7-1.8 um)
p+-a-Si:H
(15 nm)
i
a-Si:H (250- 300 nm)
n
n+-a-Si:H (30 nm)
Al or Ag
i
n
Al or Ag
Glass, plastic or
stainless steel
Opaque substrate
No light-trapping schemes: effmax~7-8%
The pp-i-n junction under illumination
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h t carrier
hot
i
E-field
E
field
Ec
photons
EFn
qV
Vph
EFn
p
Ev
Trapping
i
-
electron
hole
A
+
n
Load
I = Idiode-Iph
Simulation with AMPS program
PV performance parameters
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I
Vmax
VOC
ma
0
V
Vmax × J max
FF =
<1
J SC × VOC
Pmax
Imax
ISC
J SC × VOC × FF
=
×100 %
2
100 mW / cm
(
)
Iph
I
RS
Idiode
+
V
RLoad
L
Pout
η=
× 100 %
Poptical
RP
AM1 5 light
AM1.5
li ht
Load resistance, Rload
Solar cell
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Chemical Vapor Deposition
rf-PECVD HW-CVD
SunFab™ AMAT
Parameter
PRF
Tfil
RF or VHF
PECVD
50-700
mWcm-22
HW-CVD
HW
CVD
• Gases: SiH4, H2, PH3, B(CH3)3
• Base pressure: better than 10-5 Torr
1750-2500˚C
pw
0.1-6 Torr
10-200 mTorr
ds-e(f),
1 – 4 cm
3-7 cm
In HWCVD:
single or multi Ta or W filaments
• Tsub= 150 - 350ºC
• Substrate: glass,
glass stainless steel
steel,
plastics
• Plasma excitation frequency:
13.56 MHz, 27.12 MHz, 40.68 MHZ…
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Light--induced degradation
Light
R=
FH 2
FSiH 4
C. Wronski, 1st Intl. Workshop on Staebler-Wronski
Staebler Wronski effect, April 20-23,
20 23, 2009, Berlin
Another effect of H2 dilution
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Transport
10
Structure
DH =
6
10
-7
FH 2
FSiH 4 + FH 2
5
10
4
σph/σdk
10
DH
3
10
10
-8
95%
10
1
50
-1
-1
σd ( Ω cm )
2
10
10
10
10
-11
70
80
H2 dilution
90
100
photosensitivity
-9
9
-10
60
90%
80%
65%
50
60
70
80
H2 dilution (%)
Dark conductivity
50%
90
300 350 400 450 500 550 600
Raman Shift
Shift, cm
-1
Raman spectra
High efficiency solar cells: multijunctions
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Tandem micromorph solar cell
IMT
hν
105
glass
TCO
p
104
Absorption [1/cm]
i
103
a-Si:H
n
p
µc-Si:H
μc-Si:H
102
i
101
n
TCO
Back contact
a-Si:H
100
10
0.5
SEM micrograph
c-Si
-1
1
1.5
2
Energy [eV]
ZnO
2.5
µc- Si:H
a Si:H
a-Si:H
MicroZnO
morph
glass
INSTITUT DE
MICROTECHNIQUE
NEUCHÂTEL
Band Gapp
1.7 eV
1.1 eV
The micromorph solar cell
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High efficiency SCs: light trapping
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Single junction SC
a-Si:H
nip
n-i-p
Light
Tandem solar cell
IMT
INSTITUT DE
MICROTECHNIQUE
NEUCHÂTEL
ZnO
top cell
IR
N-layer
bottom cell
IR
a-Si:H top cell
mc-Si:H bottom cell
Ag/ZnO
T. Söderström et al, Appl. Phys. Lett. 94,
063501 (2009)
Glass
V-shape
U-shape
Matching the cell current with IR
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Flexible Solar cells on plastic
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10 W Ù 350 mW / cm2
20 W Ù 700 mW / cm2
PEN\GZO\p-RF\b-RF(9nm)\i-(350nm)\n-RF
Deposition rate (Å / s)
amorphous
4
nanocrystalline
2
5
0
-5
-10
p-i-n on PEN
p-i-n
i on PEN
-15
-1.0 -0.8 -0.6 -0.4 -0.2 0.0
0
96
97
98
98.5
99
0.2
0.4
0.6
0.8
1.0
Voltage (V)
Hydrogen dilution (%)
PEN substrates, Tsub=150ºC
100
ZnO:Ga sputtered on PEN at RT
80
%T, %R, %A
A
SC91
i-layer by HW
FF= 51.0
51 0 %
2
Jsc= -12.7 mA/cm
Voc= 0.699 V
EFF= 4.53 %
SC88
i-layer by RF
FF 54.2
FF=
54 2 %
2
Jsc= -11.2 mA/cm
Voc= 0.830 V
EFF= 5.03 %
2
6
Current Densitty (mA/cm )
C
20W,6Torr,1.2cm
10W,6Torr,1.2cm
10W 3 T
10W,3
Torr,1.2cm
12
10W,1.5Torr,1.2cm
10W,1.5Torr, 1.2cm
10
60
Transmitance
Reflectance
Absorbance
40
20
0
300
400
500
600
wavelength (nm)
700
800
Thickness
(μm)
Band
gap (eV)
1.35
1.39
Resistivity
Mobility
(cm2/ Vs)
Carrier conc.
(cm-3)
Rsh (Ω/)
ρ (Ω cm)
3.53
5.1
1 × 10-3
16.3
4.28 × 1020
3.55
3.9
7 × 10-4
17.5
5.13 × 1020
900
P. Alpuim et al., Proc. 23rd European PV Solar Energy Conference and
Exhibition (23rd EU PVSEC), Valencia, Spain (2008) 2455
Roll--toRoll
to-roll deposition of modules
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In-situm series connection (ISSC)
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Conclusions
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• Cost structure & differentiation will matter
more than before
• Direct competition with c-Si wafers PV (1st
generation PV ) will be harder
• Find niche markets, make unique products,
avoid price competition
• Improve conversion efficiency:
• R&D to improve optical part of device
• Develop multijunction devices
• Develop in
in-line
line deposition systems
Thank you for your attention!
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Record efficiencies for solar cells
and modules
Highest reported small area cell eff.
Highest reported module eff.
Type of cell
Eff.
(%)
Area
(cm2)
Reference
Type of module
Eff.
(%)
Area
(cm2)
Reference
Crystalline Si
25.0
4.0
UNSW1, PERL2
Crystalline Si
22.9
778
UNSW/Gochermann
Thin film transfer Si
16.7
4.0
U. Stuttgart
Large c-Si
20.3
16 300
SunPower
Multicrystalline Si
20.3
1.0
FhG-ISE3
Multicrystalline Si
15.3
1 017
Sandia/HEM
Nanocrystalline
N
t lli Si
Amorphous Si
10.1
10
1
9.5
1.2
1
2
1.1
K
Kaneka
k
U. Neuchatel
Thi fil
Thin
film
polycrystalline Si
82
8.2
661
P ifi S
Pacific
Solar
l
a-Si / mc-Si
11.7
14.2
Kaneka
a-Si/a-SiGe/a-SiGe
10.4
905
USSC4
CIGS
19.4
0.99
NREL5
CIGS
13.5
3 459
Showa Shell
CdTe
16.7
1.0
NREL
CdTe
10.9
4 874
BP Solarex
Organic polymer
5.1
1.0
Konarka
Organic submodule
2.1
223.5
Plextronics
1UNSW,
University of New South Wales
2PERL, passivated emitter rear locally diffused
3FhG-ISE, Fraunhofer Institute for Solar Energy Systems
4USSC,
USSC United Solar Systems Corporation
5NREL, National Renewable Energy Lab
Adapted from M.A. Green et al., Prog. Photovolt: Res. Appl. 17 (2009) 320
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