Stability and Efficiency of Organic Solar cells - Help
Transcript of Stability and Efficiency of Organic Solar cells - Help
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Vikram Dalal
Iowa State University
* Supported in part by a NSF Grant
Stability and Efficiency of Organic
Solar cells
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Acknowledgments
To M.Samiee, R. Shinar, J. Shinar, J. Bhattacharya, M. Noack,
T. Xiao, P. Joshi, M. Noack, S. Pattnaik
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Outline
Degradation – Light induced and atmospheric
Changes in fundamental material properties under
degradation
Influence of changes in contacting layers
Hybrid organic/inorganic tandem cells
Potential efficiency
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Problem
Organic cells degrade quite a bit under both light and
atmosphere
25-30% degradation in performance common; lifetime
prediction uncertain
Contrast with inorganic cells: Si cells last>30 years with
<10% degradation over that period
Can we do accelerated degradation?
What is the influence of the spectrum?
Can it be reversed?
How can we reduce degradation?
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What measurements?
Light I-V Before and after degradation
Dark I-V Before and After degradation
Quantum efficiency-Before and after
Capacitance-frequency Before and after
Mobility measurements
Degradation in light, and in air
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Experiments
Standard P3HT/PCBM cells
Glass
ITO
PEDOT/PSS or MoO3
P3HT/PCBM
Ca/Al
Light
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Exposure system-high vacuum
• Unique system
• Full spectrum AM1.5 lamp
• Intensity can be changed to ~10X
• High vacuum followed by N2/Ar
• Measurements in-situ
• Can study influence of
various gases (eg: moisture)
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Changes in performance, 2X sun intensity
Light Intensities adjusted for both cases – Current in organic cell
identical for the two cases
ORG 1023 Filter vs. No Filter
94.0%
95.0%
96.0%
97.0%
98.0%
99.0%
100.0%
101.0%
0 500 1000 1500
Time (Minutes)
% o
f In
itia
l V
alu
e
Voc Filter
Isc Filter
Voc No fi lter
Isc No fi lter
Full spectrum Xenon AM1.5
Blue a-(Si,C) filter
For accurate measurements, MUST
Use full spectrum light source!
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0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
-0.5 -0.3 -0.1 0.1 0.3 0.5
Before Exposure
After Exposure
Light I-V Slope indicates decrease in
Collection length after degradation-
More recombination
Ref. Bhattacharya et al, APL, May 2012
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Tail states and midgap states in P3HT-
measure subgap QE
1.0E-07
1.0E-06
1.0E-05
1.0E-04
1.0E-03
1.0E-02
1.0E-01
1.0E+00
0.8 1 1.2 1.4 1.6 1.8 2 2.2
Qu
antu
m e
ffic
ien
cy
Energy(eV)
BeforeDegradation
AfterDegradationTail states
Midgap
Midgap states Change, Tail states do not
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Next, interface between P3HT and
PCBM
3 measurements
C-f – gives defect density vs. energy
Dark I-V-two regions?
Dark I-V vs temperature-relationship of Jo1 vs temperature
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C-f data
Initial
With uv-blue filter
Full spectrum
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DOS of defects in another device- 5X increase
at~0.5-0.6 eV
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1.0E-11
1.0E-10
1.0E-09
1.0E-08
1.0E-07
1.0E-06
1.0E-05
1.0E-04
1.0E-03
1.0E-02
0 0.2 0.4 0.6 0.8VOLTAGE(VOLT)
After 2xIllumination for96 Hrs
Change in dark I-V-light exposure only-note the change in
earlier I-classic increasing midgap state problem:
5X increase in J01
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Dark I-V vs. Temperature-Control sample
Pre exposure – dark I-V controlled by interface-
and interface changes upon exposure
-30
-29
-28
-27
-26
-25
-24
-23
-22
-21
-20
30 32 34 36 38 40
1/kT(kT in eV)
Ln
(Io
/sq
rt(T
))
slope=0.62 eV
The slope ~ ½ of LUMO-HOMO At interface
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1.2 eV
P3HT
PCBM
LUMO level
HOMO level
P3HT/PCBM heterojunction
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Bob Street’s Data
[Street et al,AFM,2012]
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Influence of post-degradation thermal
anneal, 100 C
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Changes in defect densities upon
thermal annealing after degradation
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Next, influence of contacts
Anneal MoO3 or PEDOT/PSS at various temperatures
BEFORE depositing solar cells
Then study degradation in absence of oxygen/moisture
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Changes in Isc and efficiency vs. pre-
annealing of contacts
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McGehee group data on contacts
[Peters et al,AM,2012]
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Bob Street Group’s Data
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Conclusion on stability
UV and blue photons do much more damage than equivalent
dose of red photons
Contacts make a difference
Interface seems to be damaged
Midgap states in P3HT are also being generated by light
Thermal annealing seems to help partially
Q: Can we use a device design to not waste blue photons and
yet improve stability?
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Basic device structure: Hybrid
inorganic/organic tandem
Light
The bandgap of inorganic can
Be changed at will to match
the organic cell
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Intermediate layer-Critical:
Sputtered ITO
The intermediate layer MUST provide a good ohmic contact to the first cell,
and a good ohmic contact to the second. ITO good contact for n+ a-(Si,C)
(tunnel contact) and a good hole injector for P3HT (valence band match)
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I-V curve of the P3HT:PCBM cell by
itself.
0.0 0.2 0.4 0.60
3
6
9
12
Cu
rre
nt
De
ns
ity
(m
A/c
m2)
Voltage (V)
Organic only
FF=64%
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I-V curve of tandem
Note the voltage, ~1.5 V =
sum of amorphous + organic
Note the Fill factor, 77%- shows
No problem at interface
Between two cells
Ref: Pattnaik et al, IEEE J. Photovolt.(to be published)
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QE of 1st and 2nd solar cells – Nicely
matched
400 500 600 700
0.1
0.2
0.3
0.4
0.5
0.6
0.7
Jorg
sc = 4.97mA/cm
2
No
rmalized
EQ
E
Wavelength (nm)
Ja-(Si,C)
sc = 5.1mA/cm
2
(c)
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What potential efficiency
With the right organic cells with LOWER gap, 12 mA/cm2
seems entirely feasible with ~0.8 V
A-Si will also give 12 mA
Combine, get 12 mA, 1.7V, 0.8 FF
Eff. ~16.3%!
And better stability – two reasons
blue photons absent, and less intensity on organic
In a triple, ~10 mA, 2.7V, 0.8 FF, Eff. Of = 21.6% possible
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Influence of photonics and plasmonics
Must model it right-3D model needed – can increase current
by ~40% in P3HT
9
10
11
12
13
14
15
16
0 10 20 30 40 50 60 70 80
Variation with texture height
Jsc mA/cm2
Jsc
mA
/cm
2
height h nm
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Open questions on stability What are the kinetics of degradation telling us-how do we model
them?
What is the relationship between stability and intensity of light –model needed
How about stability and temperature effects?
Can we anneal out defects?
Is there synergy between light induced and moisture induced degradation?
How do we reduce the influence of contacts on degradation ? What new contacting layers can be used?
How does structure change in degradation? What is the influence between structural changes and electronic property changes?
How do we minimize interfacial changes?
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Open questions on multiple junction
cells
How do we optimize light collection using photonic and
plasmonic effects? Modeling and experiments needed for the
entire structure
What are the best intermediate connecting layers?
How do these layers affect stability of multi-junction cells?