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Material and Structural Designfor High Efficiency Dye-Sensitized Solar Cell
Hyungjun Koo, Beomjin Yoo, Kicheon Yoo, Kyungkon Kim and Nam-Gyu Park*
Center for Energy MaterialsKorea Institute of Science and Technology
(KIST)
N
N
C
C
O
O
HO
N
N
C
C
O
O
O
HO
RuNCS
NCS
O
The 4th US-Korea NanoForum
2
DSSC: structure and operation principle
D*/D+
D/D+
CB
VB
I3¯/I¯surface states
Voc
TiO2 Dye
τinj
τcc
τr
TCO
TiO2
N
N
C
C
O
O
HO
N
N
C
C
O
O
O
HO
RuNCS
NCS
O
3
issues
Efficiency (η) = (JscⅹVocⅹFF)/Pin
Case1: JSC increased by 30%1000.740.7518 → 23.410 →
13
cf.PinFFVocJscη (%)
Case2: VOC increased by 30%1000.740.75 → 0.981810 →
13
cf.PinFFVocJscη (%)
Efficiency (η) = (JscⅹVocⅹFF)/Pin
13%
13%
* efficiency as high as 11% has been achieved.* higher efficiency is required in order to be in competition with Si solar cell
Approaches for improving efficiency
4
light confinement by scattering:
size-dependent scattering efficiency &bi-functional material
structural and material design
strategy for improving JSC
5
nanoparticle films for DSSC
180 190 200 210 220 230 2407.0
7.5
8.0
8.5
9.0
Effic
ienc
y (%
)
Autoclave Temp. (oC)
210 220 230 2407.0
7.5
8.0
8.5
9.0
Effic
ienc
y (%
)
Autoclave Temp. (oC)
t = 5-6 µm t = 10-12 µm
Simple increase of nanoparticle film may not improve the efficiency to great extent!
6
(a) G1 (b) G2
20 25 30 35 40 45 50 55 60
(b)
R(2
20)R
(211
)
R(2
10)
R(1
11)
R(2
00)R
(101
)R(1
10)
A
***
A
Inte
nsity
(a.u
.)
2θ (degree)
(a)
size-dependent scattering efficiency
SL
7
+16.3%8.78 ± 0.0970.7 ± 0.4866 ± 114.4 ± 0.11L+G2
+18.4%8.94 ± 0.0870.4 ± 0.3852 ± 214.9 ± 0.01L+G1
7.55 ± 0.1271.1 ± 0.1868 ± 212.2 ± 0.11L (~7 µm)
Increasing rateEff. (%)FF (%)Voc (mV)Jsc
(mA/cm2)
PV properties
400 500 600 700 8000
20
40
60
80
IPC
E
Wavelength
1 L 1 L+G1 1 L+G2
8
400 500 600 700 8000
20
40
60
80
100
Ref
lect
ance
(%)
Wavelength (nm)
nano-TiO2 film G1 film G2 film
reflectance spectra
nano-TiO2thin filmunderlayer
scatteringoverlayer
9
bi-functional material* spherical or flat surface large particles are normally used for light scattering
* except light scattering, such materials do not contribute to photocurrent generation due to low surface area
* motivation: design of bi-functional material exhibiting both light scattering and photocurrent generation efficiently
Nano-Embossing Hollow Sphere TiO2(prepared by Prof. W.-I. Lee)
300 nm300 nm300 nm
10
IPCE & reflectance comparison
400 500 600 700 8000
20
40
60
80
IPC
E (%
)
Wavelength (nm)
2L 1L-NeHS 1L-CCIC
400 500 600 700 800 9000
20
40
60
80
100(b)
%R
Wavelength (nm)
CCIC TiO2 Particle Film NeHS TiO2 Film nanocrystalline TiO2 Film
1L
NeHS
11
conversion efficiency
0.0 0.2 0.4 0.6 0.80
5
10
15
20
Phot
ocur
rent
den
sity
(m
A/c
m2 )
Voltage (V)
JSC : 17.8 mA/cm2
VOC : 0.845 V FF : 0.69 η : 10.34%
without long-term post-treatment of TiCl4
12
interfacial nano-engineering
13
locus of recombination
bulkrecombination
near substraterecombination
14
methods for suppression of recombination
Mesoporous electrode
blocking layer
TiO2
FTO
TiO2FTO
core-shell
(to protect bulk recombination)
(to protect recombination at near substrate)
15
FTO/BL/TiO2: SEM
300nm
Bare
0.15 M
0.4 M
300nm
Blocking layer
TiO2FTO
Chemically formed from Ti precursor solution
16
effect of Ti-precursor concentration on PV property
0.0 0.2 0.4 0.6 0.8
12.6
12.8
13.0
13.2
13.4
0.0 0.2 0.4 0.6 0.80.80
0.82
0.84
0.86
0.88
0.0 0.2 0.4 0.6 0.80.70
0.72
0.74
0.760.0 0.2 0.4 0.6 0.8
7.6
7.8
8.0
8.2
8.4
J SC (m
A/c
m2 )
VO
C (V
)
Ti precursor concentration (M)
FF
η (%
)
measuredunder mask with aperture
17
EIS (bode plot)
10-2 10-1 100 101 102 103 104 105 1060
-10
-20
Frequency, Hz
Thet
a
100 101 102 103 104
0.8M
0.4M0.2M
0.15M0.1M0.05Mbare
CB A
2nd
deriv
ativ
e th
eta
(arb
t. un
it)
Frequency, Hz
A: pt/electrolyte; B: FTO/electrolyte; C: TiO2/dye/electrolyte
0
-5
Cole-Cole
Bode
0.0 0.5 1.010-5
10-4
10-3
Inve
rse
freq
uenc
y (1
/Hz)
Precursor concentration (M)
A
0.0 0.5 1.010-4
10-3
10-2
Precursor concentration (M)
Inve
rse
freq
uenc
y (1
/Hz)
B
0.0 0.5 1.010-2
10-1
Precursor concentration (M)
Inve
rse
freq
uenc
y (1
/Hz) C
Hz
Hz
18
Surface modification of bulk TiO2 film: fast electron transport, slow recombination
10-2 10-1 100
10-3
10-2
10-1
photocurrent transient
Tim
e (S
)
Photocurrent Density(mA/cm2)
bare TiO2 Photocurrent Photovoltage
TiO2 treated with TiCl4(9hr) Photocurrent Photovoltage
photovoltage transient
Transient photocurrentτTiCl4 treatment < τTiO2
⇒ Enhanced electron transport by TiCl4 treatment
Transient photovoltageτTiCl4 treatment > τTiO2
⇒ Reduced recombination from TiO2 to electrolyte by TiCl4 treatment
19
DSSC best efficiency
0.0 0.2 0.4 0.6 0.8 1.002468
10121416182022
Phot
ocur
rem
t den
sity
(m
A/cm
2 )
Voltage (V)
Jsc = 19.38 mA/cm2
Voc = 0.877 VFF = 0.647Eff. = 11%@ AM 1.5G-1 sun
Reference cell: NREL-calibrated mono Si with KG-5 filter
close to the world best efficiency of 11.1% from EPFL
20
PCBMP3HT
Kim et. al., APL 90, 163511 (2007)
Thickness: D1<D2<D3
Max. Eff. of 6.1% was obtained from D2
KIST Activity: Organic Photovoltaics
21
Acknowledgments
KIST Specialists Laboratory for Dye-Sensitized & Organic Solar Cells$$$: KIST, MOST and MOCIE
HJ. Koo NJ. Myung
SY. Bang, MS
KC. Yoo KT. Lee, staff
KW. Lee, MS
TR. Lee
BJ. Yoo, Ph.D.
MA. Lee, MS
Dr. K Kim, Senior Scientist