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H. Wang1, J. X. Wang1, A. B. Prakoso1,2, and Rusli 1,2
1School of Electrical and Electronic Engineering,
Nanyang Technological University, Singapore
2CINTRA UMI CNRS/NTU/THALES 3288, Research Techno
Plaza, NTU, Singapore
email: erusli@ntu.edu.sg
Thin Film Silicon Nanowire/PEDOT:PSS
Hybrid Solar Cells with Surface Treatment
1
Nanyang Technological University
Singapore
2
Outline
 Introduction
 SiNWs/PEDOT:PSS hybrid cell
 Experiments, results and discussions
 Fabrication of thin film SiNWs/PEDOT:PSS cells
 Two-step surface treatment
 Characterization of hybrid cells
 Conclusions
3
 Inorganic solar cells
 High carriers mobility
 High PCE & stability
 High material cost
 Complex fabrication
 Organic solar cells
 Low material cost
 Simple solution process
 Low carriers mobility
 Low PCE & poor lifetime
 Hybrid solar cells
 Combined advantages
Introduction
4
 Si/PEDOT:PSS hybrid cell
 Si is abundant, non-toxic
 Eg = 1.1 eV, large absorption spectrum
 PEDOT:PSS is transparent and conductive
 Si/PEDOT:PSS solar cells belong to a type of selective carriers
contact (SCC) solar cell. PEDOT:PSS serves as hole SCC and
plays passivation role.
 Large area, low temperature and solution based low cost
fabrication process. Greatly simplified compared to conventional
Si solar cells.
Introduction
5
 Si nanostructures (e.g. nanowires, nanocones and nanoholes) are
commonly introduced for light trapping and anti-reflection.
 Excellent light trapping allows use of thinner Si.
 Provide large heterojunction area.
 SiNWs/organic hybrid structure with
shorter diffusion distance
 SiNWs and SiNHs are typically fabricated
using large area, solution based, low cost
metal-catalyzed electroless etching (MCEE) technique.
 Efficiency has improved significantly in recent years from 5% to
13.0% for front-junction cell, reached 17.4% for back-junction cell.
Introduction
Si
PEDOT:PSS
6
Si
structure
Organic material Group/year PCE (%)
Jsc
(mA/cm2)
SiNW
Poly(3-octylthiophene)
(P3OT)
G. Kalita et al. /2010 [1] 0.61 7.85
SiNW PEDOT: PSS W. Lu et al./2011 [7] 6.35 21.2
SiNW PEDOT: PSS S.-J. Syu et al./2011 [8] 8.4 24.2
SiNW (P3HT) F. Zhang et al./2012 [2] 9.2 37.6
SiNW
Spiro-OMeTAD/PEDOT:
PSS
L. He et al./2011 [3] 10.3 30.9
SiNW
Spiro-OMeTAD/PEDOT:
PSS
X. Shen et al./2011 [4] 9.7 31.3
SiNW PEDOT: PSS P.C. Yu et al./2013 [5] 13.0 34.3
SiNW PEDOT: PSS R. Y. Liu et al./2014 [6] 12.0 32.3
SiNW PEDOT: PSS J. X. Wang et al./2015 [9] 12.4 30.8
SiNW
PEDOT:PSS (back
junction)
D. Zielke et al./2014 [10] 17.4 39.7
7
References
1 G. Kalita, S. Adhikari, H. R. Aryal, R. Afre, T. Soga, M. Sharon, W. Koichi, and M.
Umeno, Journal of Physics D: Applied Physics 42, 115104 (5 pp.) (2009).
2 F. Zhang, X. Han, S.-T. Lee, and B. Sun, Journal of Materials Chemistry 22, 5362-5368
(2012).
3 L. He, C. Jiang, Rusli, D. Lai, and H. Wang, Applied Physics Letters 99, 021104-6
(2011).
4 X. Shen, B. Sun, D. Liu, and S.-T. Lee, Journal of the American Chemical Society 133,
19408-19415 (2011).
5 P. C. Yu, C. Y. Tsai, J. K. Chang, C. C. Lai, P. H. Chen, Y. C. Lai, P. T. Tsai, M. C. Li, H.
T. Pan, Y. Y. Huang, C. I. Wu, Y. L. Chueh, S. W. Chen, C. H. Du, S. F. Horng, H. F.
Meng, Acs Nano 7, 10780-10787 (2013).
6 R. Y. Liu, S. T. Lee, and B. Q. Sun, Advanced materials 26, 6007-6012 (2014).
7 W. Lu, C. Wang, W. Yue, and L. Chen, Nanoscale 3, 3631-3634 (2011).
8 H.-J. Syu, S.-C. Shiu, and C.-F. Lin, Solar Energy Materials and Solar Cells 98, 267-272
(2012).
9 Jianxiong Wang et. al, Nanoscale, Vol 7, 4559-65 (2015)
10 D. Zielke, A. Pazidis, F.Werner and J. Schmidt, Solar Energy Materials &Solar Cell 131,
110-116 (2014).
8
Hybrid Si/PEDOT:PSS Solar Cells
Year Strucutre PCE (%)
2011 SiNW/SPIRO hybrid cell1 10.3
2011 SiNW/PEDOT hybrid cell2 9.0
2012 Pymarids/SiNWs/PEDOT hybrid solar cells3 9.9
2012 Planar Si/PEDOT hybrid cell4 10.6
2012 SiNWs/ PEDOT hybrid cell with 2.2um epitaxial Si5
5.6
2014 SiNH/PEDOT hybrid cell6 8.3
2015 SiNW/PEDOT hybrid cell with surface treatment7 12.4
2016 Planar Si/PEDOT hybrid cell with 15.5um epitaxial Si8 8.7
2016 SiNH/PEDOT hybrid cell9 12.9
1 L. He et. al, Applied Physics Letters 99, 021104-6 (2011).
2 L. He et. al, IEEE Electron Device Letters, 32, pp. 1406-8 (2011).
3 L. He et. al, Small, vol 8, pp. 1664-1668, (2012).
4 L. He et. al, Applied Physics Letters, vol. 100, pp. 073503-5 (2012).
5 L. He et. al, Applied Physics Letters, vol 100, pp. 103104-7 (2012)
6 L. Hong et. al, Applied Physics Letters, vol 104, 053104 (2014)
7 J. X. Wang et. al, Nanoscale, Vol 7, 4559-65 (2015)
8 H. Wang et al, IEEE Journal of Photovoltaics 6, 217 (2016).
9 Z. Y. Li et. al, EU PVSEC (2016)
9
Hybrid Si/PEDOT:PSS Solar Cells
SiNWs/PEDOT:PSS
Solar Cells
Pyramid/SiNWs/PEDOT:PSS
Solar Cells
SiNHs/PEDOT:PSS
Solar Cells
10
 The efficiencies of hybrid solar cell based on Si
nanostructures are not much better than planar cell,
despite their excellent light trapping properties.
 Jsc is increased but Voc is substantially lowered.
 Attributed to the severe carriers recombination
associated with the defective surface.
Introduction
11
 Defective SiNWs surface
 Dry etching ion bombard damage of the surface
 Metal catalyze electroless etching (MCEE)
 Large surface area of the nanostructures
 PEDOT:PSS layer is not fully penetrated into the gaps
of SiNWs
 Long molecular chain of PEDOT:PSS and its fast
drying process
 Agglomeration of the long nanowires
Introduction
12
 Various approaches can reduce the recombination of
nanostructures
 Surface passivation
 Attaching some chemical molecules to the Si surface.
E.g. CH3-temination
 Using native oxides as passivation layer. SiOx have
been commonly used for passivation.
 Optimized nanostructures
 Shrinking surface area but not sacrificing their light
absorption. (e.g. inverted nanopyramid, nanoholes)
Introduction
13
Nanowires/PEDOT:PSS
hybrid cells on thin film Si with
surface treatment
14
 We applied a two-step surface treatment to hybrid
SiNWs/PEDOT:PSS solar cells.
 Treated with O2 plasma surface treatment to grow oxide,
which embeds the Ag nanoparticles. Oxide is then
partially removed and leave behind a thin layer for
passivation.
 Si/PEDOT:PSS hybrid cells are demonstrated on thin
film Si to lower the material cost.
 SiNWs with different lengths are investigated.
Introduction
15
Fabrication Process
16
Fabrication Details
 10.6 µm epitaxial single crystal (100) Si film grown by HTCVD on
n++ Si (100) substrates using dichlorosilane precursor and
phosphine (PH3) dopant gas at 1000 oC.
 MCEE: etching solution of 4.6 M HF and 0.02 M AgNO3 at room
temperature to fabricate the SiNWs
 SiNWs
 Length: 0.4 to 2.7 µm
 Diameter: 20 to 100 nm
 Gap between SiNWs: < 50 nm
 O2 plasma treatment 480 sec : 30 sccm, RF power of 30 watts and
pressure of 200 mTorr.
 SiNWs were etched in a 5% HF solution for 85 s to reduce the
thickness of the surface oxide and obtain a cleaner surface
 PEDOT:PSS thickness: 80 mn
 Back contact Ti/Pd/Ag: 50nm : 50nm : 1000 nm
 Front contact Ag: 1000 nm
 Active area of cell: 0.95 cm2.
17
Epitaxial Si films
DSIMS profile XRD spectrum
 Doping concentration of Si film: of ~ 1.5×1016 cm-3.
 Thickness (T) of Si film is 10.6 µm
 Doping concentration of substrate: of ~ 1×1020 cm-3.
Photocurrrent generation takes place only in the 10.6 µm Si
absorber layer
18
SEM image of the hybrid cells
top view
cross-section cross-section
 Longer SiNWs suffer from agglomeration at the top resulting in the
formation of large bundles of SiNWs, ascribed to the Van Der Walls
and attractive capillary forces
19
SEM image of the hybrid cells
top view
 Treated SiNWs reveal a smoother surface coverage of
PEDOT:PSS layer 20
untreated treated untreated treated
before treatment
(hydrophobic)
Contact angle measurement of SiNW
substrate
 Smoother surface of treated cell is attributed to O2 plasma
treatment that resulted in a more hydrophilic surface.
 This facilitates better coverage of PEDOT:PSS on the surface of the
SiNWs and better penetration into the gaps between the SiNWs
after HF etching
(hydrophilic)
after treatment
(hydrophilic)
21
 Reflectance drops with increasing L.
 The EQE peak increases with L up to L = 0.95 µm, with a maximum
value of 69.7% at λ = 625 nm. Attributed to the enhanced light
trapping and charge separation capability of the SiNWs.
 As L further increases to 1.5 and 2.7 µm, EQE drops due to the
higher surface recombination with the SiNWs bundles.
External Quantum Efficiency
400 600 800 1000
0
20
40
60
80
EQE(%)
Wavelength (nm)
0.4 µm
0.7 µm
0.95 µm
1.5 µm
2.7 µm
(a)
400 600 800 1000
0
10
20
30
40
50
Reflectance(%)
Wavelength (nm)
0.4 µm
0.7 µm
0.95 µm
1.5 µm
2.7 µm
(b)
22
J-V Characteristics of Hybrid Cells
0.0 0.2 0.4 0.6
-20
-15
-10
-5
0
Voc (V) Jsc (mA/cm2) FF(%) PCE(%)
Untreated 0.496 20.6 68.6 7.02
Treated 0.572 20.6 65.7 7.74
CurrentDensity(mA/cm
2
)
Voltage (V)
0.4µm Untreated
0.4µm Treated
(a)
0.0 0.2 0.4
-20
-15
-10
-5
0
Voc (V) Jsc (mA/cm2) FF(%) PCE(%)
Untreated 0.416 20.3 51.7 4.36
Treated 0.542 21.0 63.7 7.24
(b)
CurrentDensity(mA/cm
2
)
Voltage (V)
0.95µm Untreated
0.95µm Treated
 Voc of treated cell is recovered to 0.572 V and 0.542 V, much higher
than the untreated cell.
 Jsc and FF also improved for longer wires.
23
0.5 1.0 1.5 2.0 2.5 3.0
0.2
0.4
0.6
(b)
Voc(V) SiNWs length (µm)
Untreated
Treated
0.5 1.0 1.5 2.0 2.5 3.0
0
2
4
6
8
10
(a)
PCE(%)
SiNWs length (µm)
Untreated
Treated
0.5 1.0 1.5 2.0 2.5 3.0
30
40
50
60
70
80
(d)
FF(%)
SiNWs length (µm)
Untreated
Treated
0.5 1.0 1.5 2.0 2.5 3.0
10
15
20
25
(c)
Jsc(mA/cm
2
)
SiNWs length (µm)
Untreated
Treated
 Max average
PCE: 7.27% at
0.7 µm.
 PCE less
sensitive to
SiNW length
 Improvement
in Voc for all L
 Improvement in
Jsc and FF for
longer L due to
the large surface
area. Smoother
surface coverage
Performance of hybrid SiNWs Cells
25
TEM of SiNWs
EELS results
 TEM and EELS results indicate silver particles attached on SiNWs after the
MCEE process. These are difficult to remove using nitric acid even for 4 hrs.
 After O2 plasma treatment, SiOx will form and act as a sacrificial
layer to remove the silver particles and defects and achieve
cleaner SiNWs
Before treatment After treatment
26
TEM results
HRTEM characteristic of SiNWs
Before O2 plasma
treatment
After O2 plasma
treatment
After HF etching
 As prepared SiNWs have H+ terminate surface with very thin SiOx
layer
 O2 plasma treatment increases the thickness of oxide layer to 5 nm
 After HF etching, a residual 1 - 2 nm thin SiOx layer is seen on the
SiNW surface for passivation.
27
 Demonstrated a two-step surface treatment process to remove
residual impurities and defects near the SiNWs surface, and
effectively passivates the SiNWs to reduce the recombination
loss.
 Treated SiNWs hybrid solar cell reveals a high PCE of 7.83%,
and the highest ever reported Voc of 0.572 V, for 0.7 µm SiNWs
based on a 10.6 µm thin Si film.
 The proposed simple approach of surface treatment is
promising in boosting the efficiency of SiNW/organic hybrid cell
and will potentially lead to their practical use.
Conclusions
28
29

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Thin Film Silicon Nanowire - Prof.Rusli

  • 1. H. Wang1, J. X. Wang1, A. B. Prakoso1,2, and Rusli 1,2 1School of Electrical and Electronic Engineering, Nanyang Technological University, Singapore 2CINTRA UMI CNRS/NTU/THALES 3288, Research Techno Plaza, NTU, Singapore email: erusli@ntu.edu.sg Thin Film Silicon Nanowire/PEDOT:PSS Hybrid Solar Cells with Surface Treatment 1
  • 3. Outline  Introduction  SiNWs/PEDOT:PSS hybrid cell  Experiments, results and discussions  Fabrication of thin film SiNWs/PEDOT:PSS cells  Two-step surface treatment  Characterization of hybrid cells  Conclusions 3
  • 4.  Inorganic solar cells  High carriers mobility  High PCE & stability  High material cost  Complex fabrication  Organic solar cells  Low material cost  Simple solution process  Low carriers mobility  Low PCE & poor lifetime  Hybrid solar cells  Combined advantages Introduction 4
  • 5.  Si/PEDOT:PSS hybrid cell  Si is abundant, non-toxic  Eg = 1.1 eV, large absorption spectrum  PEDOT:PSS is transparent and conductive  Si/PEDOT:PSS solar cells belong to a type of selective carriers contact (SCC) solar cell. PEDOT:PSS serves as hole SCC and plays passivation role.  Large area, low temperature and solution based low cost fabrication process. Greatly simplified compared to conventional Si solar cells. Introduction 5
  • 6.  Si nanostructures (e.g. nanowires, nanocones and nanoholes) are commonly introduced for light trapping and anti-reflection.  Excellent light trapping allows use of thinner Si.  Provide large heterojunction area.  SiNWs/organic hybrid structure with shorter diffusion distance  SiNWs and SiNHs are typically fabricated using large area, solution based, low cost metal-catalyzed electroless etching (MCEE) technique.  Efficiency has improved significantly in recent years from 5% to 13.0% for front-junction cell, reached 17.4% for back-junction cell. Introduction Si PEDOT:PSS 6
  • 7. Si structure Organic material Group/year PCE (%) Jsc (mA/cm2) SiNW Poly(3-octylthiophene) (P3OT) G. Kalita et al. /2010 [1] 0.61 7.85 SiNW PEDOT: PSS W. Lu et al./2011 [7] 6.35 21.2 SiNW PEDOT: PSS S.-J. Syu et al./2011 [8] 8.4 24.2 SiNW (P3HT) F. Zhang et al./2012 [2] 9.2 37.6 SiNW Spiro-OMeTAD/PEDOT: PSS L. He et al./2011 [3] 10.3 30.9 SiNW Spiro-OMeTAD/PEDOT: PSS X. Shen et al./2011 [4] 9.7 31.3 SiNW PEDOT: PSS P.C. Yu et al./2013 [5] 13.0 34.3 SiNW PEDOT: PSS R. Y. Liu et al./2014 [6] 12.0 32.3 SiNW PEDOT: PSS J. X. Wang et al./2015 [9] 12.4 30.8 SiNW PEDOT:PSS (back junction) D. Zielke et al./2014 [10] 17.4 39.7 7
  • 8. References 1 G. Kalita, S. Adhikari, H. R. Aryal, R. Afre, T. Soga, M. Sharon, W. Koichi, and M. Umeno, Journal of Physics D: Applied Physics 42, 115104 (5 pp.) (2009). 2 F. Zhang, X. Han, S.-T. Lee, and B. Sun, Journal of Materials Chemistry 22, 5362-5368 (2012). 3 L. He, C. Jiang, Rusli, D. Lai, and H. Wang, Applied Physics Letters 99, 021104-6 (2011). 4 X. Shen, B. Sun, D. Liu, and S.-T. Lee, Journal of the American Chemical Society 133, 19408-19415 (2011). 5 P. C. Yu, C. Y. Tsai, J. K. Chang, C. C. Lai, P. H. Chen, Y. C. Lai, P. T. Tsai, M. C. Li, H. T. Pan, Y. Y. Huang, C. I. Wu, Y. L. Chueh, S. W. Chen, C. H. Du, S. F. Horng, H. F. Meng, Acs Nano 7, 10780-10787 (2013). 6 R. Y. Liu, S. T. Lee, and B. Q. Sun, Advanced materials 26, 6007-6012 (2014). 7 W. Lu, C. Wang, W. Yue, and L. Chen, Nanoscale 3, 3631-3634 (2011). 8 H.-J. Syu, S.-C. Shiu, and C.-F. Lin, Solar Energy Materials and Solar Cells 98, 267-272 (2012). 9 Jianxiong Wang et. al, Nanoscale, Vol 7, 4559-65 (2015) 10 D. Zielke, A. Pazidis, F.Werner and J. Schmidt, Solar Energy Materials &Solar Cell 131, 110-116 (2014). 8
  • 9. Hybrid Si/PEDOT:PSS Solar Cells Year Strucutre PCE (%) 2011 SiNW/SPIRO hybrid cell1 10.3 2011 SiNW/PEDOT hybrid cell2 9.0 2012 Pymarids/SiNWs/PEDOT hybrid solar cells3 9.9 2012 Planar Si/PEDOT hybrid cell4 10.6 2012 SiNWs/ PEDOT hybrid cell with 2.2um epitaxial Si5 5.6 2014 SiNH/PEDOT hybrid cell6 8.3 2015 SiNW/PEDOT hybrid cell with surface treatment7 12.4 2016 Planar Si/PEDOT hybrid cell with 15.5um epitaxial Si8 8.7 2016 SiNH/PEDOT hybrid cell9 12.9 1 L. He et. al, Applied Physics Letters 99, 021104-6 (2011). 2 L. He et. al, IEEE Electron Device Letters, 32, pp. 1406-8 (2011). 3 L. He et. al, Small, vol 8, pp. 1664-1668, (2012). 4 L. He et. al, Applied Physics Letters, vol. 100, pp. 073503-5 (2012). 5 L. He et. al, Applied Physics Letters, vol 100, pp. 103104-7 (2012) 6 L. Hong et. al, Applied Physics Letters, vol 104, 053104 (2014) 7 J. X. Wang et. al, Nanoscale, Vol 7, 4559-65 (2015) 8 H. Wang et al, IEEE Journal of Photovoltaics 6, 217 (2016). 9 Z. Y. Li et. al, EU PVSEC (2016) 9
  • 10. Hybrid Si/PEDOT:PSS Solar Cells SiNWs/PEDOT:PSS Solar Cells Pyramid/SiNWs/PEDOT:PSS Solar Cells SiNHs/PEDOT:PSS Solar Cells 10
  • 11.  The efficiencies of hybrid solar cell based on Si nanostructures are not much better than planar cell, despite their excellent light trapping properties.  Jsc is increased but Voc is substantially lowered.  Attributed to the severe carriers recombination associated with the defective surface. Introduction 11
  • 12.  Defective SiNWs surface  Dry etching ion bombard damage of the surface  Metal catalyze electroless etching (MCEE)  Large surface area of the nanostructures  PEDOT:PSS layer is not fully penetrated into the gaps of SiNWs  Long molecular chain of PEDOT:PSS and its fast drying process  Agglomeration of the long nanowires Introduction 12
  • 13.  Various approaches can reduce the recombination of nanostructures  Surface passivation  Attaching some chemical molecules to the Si surface. E.g. CH3-temination  Using native oxides as passivation layer. SiOx have been commonly used for passivation.  Optimized nanostructures  Shrinking surface area but not sacrificing their light absorption. (e.g. inverted nanopyramid, nanoholes) Introduction 13
  • 14. Nanowires/PEDOT:PSS hybrid cells on thin film Si with surface treatment 14
  • 15.  We applied a two-step surface treatment to hybrid SiNWs/PEDOT:PSS solar cells.  Treated with O2 plasma surface treatment to grow oxide, which embeds the Ag nanoparticles. Oxide is then partially removed and leave behind a thin layer for passivation.  Si/PEDOT:PSS hybrid cells are demonstrated on thin film Si to lower the material cost.  SiNWs with different lengths are investigated. Introduction 15
  • 17. Fabrication Details  10.6 µm epitaxial single crystal (100) Si film grown by HTCVD on n++ Si (100) substrates using dichlorosilane precursor and phosphine (PH3) dopant gas at 1000 oC.  MCEE: etching solution of 4.6 M HF and 0.02 M AgNO3 at room temperature to fabricate the SiNWs  SiNWs  Length: 0.4 to 2.7 µm  Diameter: 20 to 100 nm  Gap between SiNWs: < 50 nm  O2 plasma treatment 480 sec : 30 sccm, RF power of 30 watts and pressure of 200 mTorr.  SiNWs were etched in a 5% HF solution for 85 s to reduce the thickness of the surface oxide and obtain a cleaner surface  PEDOT:PSS thickness: 80 mn  Back contact Ti/Pd/Ag: 50nm : 50nm : 1000 nm  Front contact Ag: 1000 nm  Active area of cell: 0.95 cm2. 17
  • 18. Epitaxial Si films DSIMS profile XRD spectrum  Doping concentration of Si film: of ~ 1.5×1016 cm-3.  Thickness (T) of Si film is 10.6 µm  Doping concentration of substrate: of ~ 1×1020 cm-3. Photocurrrent generation takes place only in the 10.6 µm Si absorber layer 18
  • 19. SEM image of the hybrid cells top view cross-section cross-section  Longer SiNWs suffer from agglomeration at the top resulting in the formation of large bundles of SiNWs, ascribed to the Van Der Walls and attractive capillary forces 19
  • 20. SEM image of the hybrid cells top view  Treated SiNWs reveal a smoother surface coverage of PEDOT:PSS layer 20 untreated treated untreated treated
  • 21. before treatment (hydrophobic) Contact angle measurement of SiNW substrate  Smoother surface of treated cell is attributed to O2 plasma treatment that resulted in a more hydrophilic surface.  This facilitates better coverage of PEDOT:PSS on the surface of the SiNWs and better penetration into the gaps between the SiNWs after HF etching (hydrophilic) after treatment (hydrophilic) 21
  • 22.  Reflectance drops with increasing L.  The EQE peak increases with L up to L = 0.95 µm, with a maximum value of 69.7% at λ = 625 nm. Attributed to the enhanced light trapping and charge separation capability of the SiNWs.  As L further increases to 1.5 and 2.7 µm, EQE drops due to the higher surface recombination with the SiNWs bundles. External Quantum Efficiency 400 600 800 1000 0 20 40 60 80 EQE(%) Wavelength (nm) 0.4 µm 0.7 µm 0.95 µm 1.5 µm 2.7 µm (a) 400 600 800 1000 0 10 20 30 40 50 Reflectance(%) Wavelength (nm) 0.4 µm 0.7 µm 0.95 µm 1.5 µm 2.7 µm (b) 22
  • 23. J-V Characteristics of Hybrid Cells 0.0 0.2 0.4 0.6 -20 -15 -10 -5 0 Voc (V) Jsc (mA/cm2) FF(%) PCE(%) Untreated 0.496 20.6 68.6 7.02 Treated 0.572 20.6 65.7 7.74 CurrentDensity(mA/cm 2 ) Voltage (V) 0.4µm Untreated 0.4µm Treated (a) 0.0 0.2 0.4 -20 -15 -10 -5 0 Voc (V) Jsc (mA/cm2) FF(%) PCE(%) Untreated 0.416 20.3 51.7 4.36 Treated 0.542 21.0 63.7 7.24 (b) CurrentDensity(mA/cm 2 ) Voltage (V) 0.95µm Untreated 0.95µm Treated  Voc of treated cell is recovered to 0.572 V and 0.542 V, much higher than the untreated cell.  Jsc and FF also improved for longer wires. 23
  • 24. 0.5 1.0 1.5 2.0 2.5 3.0 0.2 0.4 0.6 (b) Voc(V) SiNWs length (µm) Untreated Treated 0.5 1.0 1.5 2.0 2.5 3.0 0 2 4 6 8 10 (a) PCE(%) SiNWs length (µm) Untreated Treated 0.5 1.0 1.5 2.0 2.5 3.0 30 40 50 60 70 80 (d) FF(%) SiNWs length (µm) Untreated Treated 0.5 1.0 1.5 2.0 2.5 3.0 10 15 20 25 (c) Jsc(mA/cm 2 ) SiNWs length (µm) Untreated Treated  Max average PCE: 7.27% at 0.7 µm.  PCE less sensitive to SiNW length  Improvement in Voc for all L  Improvement in Jsc and FF for longer L due to the large surface area. Smoother surface coverage Performance of hybrid SiNWs Cells 25
  • 25. TEM of SiNWs EELS results  TEM and EELS results indicate silver particles attached on SiNWs after the MCEE process. These are difficult to remove using nitric acid even for 4 hrs.  After O2 plasma treatment, SiOx will form and act as a sacrificial layer to remove the silver particles and defects and achieve cleaner SiNWs Before treatment After treatment 26 TEM results
  • 26. HRTEM characteristic of SiNWs Before O2 plasma treatment After O2 plasma treatment After HF etching  As prepared SiNWs have H+ terminate surface with very thin SiOx layer  O2 plasma treatment increases the thickness of oxide layer to 5 nm  After HF etching, a residual 1 - 2 nm thin SiOx layer is seen on the SiNW surface for passivation. 27
  • 27.  Demonstrated a two-step surface treatment process to remove residual impurities and defects near the SiNWs surface, and effectively passivates the SiNWs to reduce the recombination loss.  Treated SiNWs hybrid solar cell reveals a high PCE of 7.83%, and the highest ever reported Voc of 0.572 V, for 0.7 µm SiNWs based on a 10.6 µm thin Si film.  The proposed simple approach of surface treatment is promising in boosting the efficiency of SiNW/organic hybrid cell and will potentially lead to their practical use. Conclusions 28
  • 28. 29