(1) The document discusses loss mechanisms in polymer-fullerene solar cells that limit performance.
(2) With additive, nongeminate recombination occurs via free carrier and trap-assisted recombination. Reconstruction works well.
(3) Without additive, incomplete reconstruction is due to voltage-dependent photogeneration from spatial trapping on fullerene islands.
1. Loss mechanisms
in Polymer-Fullerene Solar Cells
Carsten Deibel
Julius-Maximilians-University of Würzburg
223rd ECS meeting, Toronto
15th May 2013
deibel@disorderedmatter.eu
2. How Do Organic Solar Cells Work?
2
Step 1: Light Absorption
➟ Exciton Generation in Polymer
Fullerene
Aluminium Cathode
Transparent Anode
Polymer
Voltage
Current
3. How Do Organic Solar Cells Work?
3
Step 2: Exciton Diffusion
➟ to Acceptor Interface
Fullerene
Aluminium Cathode
Transparent Anode
Polymer
Voltage
Current
singlet losses
4. Step 3: Exciton Dissociation
➟ Polaron Pair Generation
How Do Organic Solar Cells Work?
4
Fullerene
Aluminium Cathode
Transparent Anode
Polymer
charge transfer:
very fast and
very efficient
Voltage
Current
singlet losses
5. How Do Organic Solar Cells Work?
5
Step 4: Polaron Pair Dissociation
➟ Free Electron–Hole Pairs!
Fullerene
Aluminium Cathode
Transparent Anode
Polymer
Voltage
Current
singlet losses
geminate losses
6. How Do Organic Solar Cells Work?
6
Step 5: Charge Transport
➟ Photocurrent
Fullerene
Aluminium Cathode
Transparent Anode
Polymer
Voltage
Current
singlet losses
geminate losses
nongeminate losses
7. for instance, PTB7:PC70BM 1:1.5
What are we looking at?
7
glass
PEDOT
V
additive DIO
8. for instance, PTB7:PC70BM 1:1.5
What are we looking at?
7
300
200
100
0
-100
currentdensity[A/m
2
]
0.80.60.40.20.0
voltage [V]
dark 1 sun
w/o add
with add
PCE [%] FF [%]
w/o add 3.8 51
with add 7.1 69
glass
PEDOT
V
15. j(V ) = e
Z
(G R) dx
⇡ jgen jloss(V )
jgen ⇡ jsc
Current–Voltage Reconstruction ...
11
From the continuity equation:
Voltage
Current
jloss(V ) /
n(V )
⌧(n)
16. 12
n(V) by charge extraction
act of Solvent Additive on PTB7:PC71BM Solar Cells 65
2
4
10
21
2
4
10
22
0.80.60.40.20.0
voltage [V]
10
21
2
4
10
22
2
4
chargecarrierdensity[m
-3
]
with add
w/o add
0.03 sun
1 sun
: Voltage dependent charge carrier density n(V ) from charge ex-
periments for PTB7:PC71BM devices with and without additive at
Alex Förtig
jloss(V ) /
n(V )
⌧(n)
Nongem. Loss Current
17. τ(n) by transient photovoltage
12
n(V) by charge extraction
act of Solvent Additive on PTB7:PC71BM Solar Cells 65
2
4
10
21
2
4
10
22
0.80.60.40.20.0
voltage [V]
10
21
2
4
10
22
2
4
chargecarrierdensity[m
-3
]
with add
w/o add
0.03 sun
1 sun
: Voltage dependent charge carrier density n(V ) from charge ex-
periments for PTB7:PC71BM devices with and without additive at
with add.
4
6
8
10
2
4
6
8
100
lifetime[µs]
3 4 5 6 7 8 9
10
22
2
charge carrier density [m
-3
]
1sun
1sun
w/out add.
Alex Förtig
jloss(V ) /
n(V )
⌧(n)
Nongem. Loss Current
18. reconstruction works well
... with Additive
Origin of nongeminate
recombination?
13
-150
-100
-50
0
50
CurrentDensity[A/m
2
]
0.60.40.20.0
Voltage [V]
meas. PL reconstr.
1 sun
0.32 sun
0.03 sun
Alex Förtig
19. LUMO
HOMO
(1)
(2)
(1)
expected in nongeminate loss in low mobility materials
Langevin Recombination
(1) finding of charge carriers → mobility μ
(2) recombination event (faster than (1))
14
R(n) / µ(n)n2
}
29. PTB7:PC70BM 1:1.5 w/o additive
I–V Reconstruction
Why?
19
reconstruction incomplete
j(V ) = jsc jloss (n(V ))
-50
-40
-30
-20
-10
0
10
CurrentDensity[A/m
2
]
0.80.60.40.2
Voltage [V]
meas. PL reconstr.
0.56 sun
0.32 sun
0.18 sun
0.03 sun
30. PTB7:PC70BM 1:1.5 w/o additive
I–V Reconstruction
Why?
19
reconstruction incomplete
j(V ) = jsc jloss (n(V ))
-50
-40
-30
-20
-10
0
10
CurrentDensity[A/m
2
]
0.80.60.40.2
Voltage [V]
meas. PL reconstr.
0.56 sun
0.32 sun
0.18 sun
0.03 sun
1.0
0.8
0.6
0.4
0.2
measured/reconstructed
0.80.60.40.2
Voltage [V]
ratio PL Voc
0.03 sun
0.18 sun
0.32 sun
0.56 sun
1 sun
First try:
31. Time Delayed Collection Field → P(V)
Main Reason: Photogeneration
w/out additive: voltage
dependent photogeneration
20Alex Förtig
5
6
7
8
9
1
Qtot/Q(-5V)
-5 -4 -3 -2 -1 0
prebias voltage [V]
w/o add
data
fit
with add
data origin unclear
32. j(V ) = e
Z
(G R) dx
⇡ jgen jloss(V )
jgen ⇡ jsc
Current–Voltage Reconstruction ...
21
From the continuity equation:
Voltage
Current
jloss(V ) /
n(V )
⌧(n)
33. j(V ) = e
Z
(G R) dx
⇡ jgen(V ) jloss(V )
Current–Voltage Reconstruction ...
22
From the continuity equation:
jloss(V ) /
n(V )
⌧(n)
Voltage
Current
jgen(V ) ⇡ jsc · P(V )
34. Time Delayed Collection Field
Reconstruction incl. Geminate Loss
23
5
6
7
8
9
1
Qtot/Q(-5V)
-5 -4 -3 -2 -1 0
prebias voltage [V]
w/o add
data
fit
with add
data
35. Time Delayed Collection Field
Reconstruction incl. Geminate Loss
23
5
6
7
8
9
1
Qtot/Q(-5V)
-5 -4 -3 -2 -1 0
prebias voltage [V]
w/o add
data
fit
with add
data
-80
-60
-40
-20
0
currentdensity[A/m
2
]
0.80.60.40.2
voltage [V]
0.18 sun
1 sun
w/o Add
measurement
reconstruction
j (V)gen
43. Thanks to Prof.
Dyakonov and
Würzburg group!
Thank you!
deibel@disorderedmatter.eu
Bayerische
Akademie der Wissenschaften
EU, DBU, Elite network Bavaria