Hybrid Si/poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate) (PEDOT:PSS) solar cells based on nanowire array structures with radial and axial junctions are prepared and investigated. Compared to axial junction cells, radial junction cells exhibit much higher external quantum efficiency for long wavelength light due to improved separation of photogenerated charge carriers, resulting in more than 10 times higher power conversion efficiency (PCE). By tuning the height of nanowire array for the hybrid radial junction cells and investigating the external quantum efficiency and open circuit voltage decay, we identify that inefficient carrier collection due to interfacial recombination is the major limiting factor for the hybrid radial junction cell performance.

1.
L.
Hu
and
G.
Chen
,
Nano Lett.
7
,
3249
(
2007
).
2.
J.
Zhu
,
Z. F.
Yu
,
G. F.
Burkhard
,
C. M.
Hsu
,
S. T.
Connor
,
Y. Q.
Xu
,
Q.
Wang
,
M.
McGehee
,
S. H.
Fan
, and
Y.
Cui
,
Nano Lett.
9
,
279
(
2009
).
3.
J. S.
Li
,
H. Y.
Yu
,
S. M.
Wong
,
G.
Zhang
,
X. W.
Sun
,
P. G. Q.
Lo
, and
D. L.
Kwong
,
Appl. Phys. Lett.
95
,
033102
(
2009
).
4.
S. E.
Han
and
G.
Chen
,
Nano Lett.
10
,
1012
(
2010
).
5.
E.
Garnett
and
P. D.
Yang
,
Nano Lett.
10
,
1082
(
2010
).
6.
W. Q.
Xie
,
W. F.
Liu
,
J. I.
Oh
, and
W. Z.
Shen
,
Appl. Phys. Lett.
99
,
033107
(
2011
).
7.
B. M.
Kayes
,
H. A.
Atwater
, and
N. S.
Lewis
,
J. Appl. Phys.
97
,
114302
(
2005
).
8.
K. Q.
Peng
,
X.
Wang
,
X. L.
Wu
, and
S. T.
Lee
,
Nano Lett.
9
,
3704
(
2009
).
9.
Y. M. C.
Putnam
,
S. W.
Boettcher
,
M. D.
Kelzenberg
,
D. B.
Turner-Evans
,
J. M.
Spurgeon
,
E. L.
Warren
,
R. M.
Briggs
,
N. S.
Lewis
, and
H. A.
Atwater
,
Energy Environ. Sci.
3
,
1037
(
2010
).
10.
F. T.
Zhang
,
B. Q.
Sun
,
T.
Song
,
X. L.
Zhu
, and
S. T.
Lee
,
Chem. Mater.
23
,
2084
(
2011
).
11.
S. C.
Shiu
,
J. J.
Chao
,
S. C.
Hung
,
C. L.
Yeh
, and
C. F.
Lin
,
Chem. Mater.
22
,
3108
(
2010
).
12.
W. H.
Lu
,
C. W.
Wang
,
W.
Yue
, and
L. W.
Chen
,
Nanoscale
3
,
3631
(
2011
).
13.
M. L.
Zhang
,
K. Q.
Peng
,
X.
Fan
,
J. S.
Jie
,
R. Q.
Zhang
,
S. T.
Lee
, and
N. B.
Wong
,
J. Phys. Chem. C
112
,
4444
(
2008
).
14.
M. A.
Green
,
Sol. Energy Mater. Sol. Cells
92
,
1305
(
2008
).
15.
The Voc decay is measured using a 635 nm laser diode illumination driven with 5 ms square pulse signals provided by a signal generator. The rise/fall time of the light pulse is less than 500 ns as tested by a high-speed photodetector (DET100A/M, Thorlabs). The transient Voc signal of the hybrid solar cells is recorded by a digitizing oscilloscope with 1 MΩ input impedance.
16.
For quasi-equilibrium states in Si nanowires, p(t)n(t)=p0n0exp[(EFn-EFp)/(kBT)] in which kBT is the thermal energy, p(t) is the hole concentration, n(t) is the electron concentration, p0 is the hole concentration for the equilibrium state in dark, n0 is the electron concentration for the equilibrium state in dark, EFp is the hole quasi-Fermi level, and EFn is the electron quasi-Fermi level. For the n-type Si nanowires, n(t)n0. Therefore, the Voc can be expressed as VOC(t)=(EFn-EFp)/q=(kBT/q)ln[p(t)/p0], where q is the positive elementary charge.
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