Combining randomly textured surfaces and one-dimensional photonic
crystals as efficient light-trapping structures in hydrogenated
amorphous silicon solar cells
Peizhuan Chen
a,b
, Guofu Hou
a,
n
, Qihua Fan
c
, Jian Ni
a
, Jianjun Zhang
a
, Qian Huang
a
,
Xiaodan Zhang
a
, Ying Zhao
a
a
Institute of Photoelectronics, Tianjin Key Laboratory of Photoelectronic Thin-film Devices and Technique, Nankai University, Tianjin 300071, PR China
b
School of Electrical Engineering & Automation, Tianjin Polytechnic University, Tianjin 300387, PR China
c
Department of Electrical Engineering and Computer Science, South Dakota State University, Brookings, SD 57007, USA
article info
Article history:
Received 16 June 2015
Accepted 25 June 2015
Keywords:
Thin-film silicon solar cell
Light trapping
Photonic crystal
Back reflector
abstract
One of the foremost challenges in achieving high-efficiency thin-film silicon solar cells is in devising an
efficient light trapping system because of the short optical path length imposed by the inherent thin
absorption layers. In this paper, an efficient light trapping system is proposed using a combination of
randomly textured surfaces and a one-dimensional photonic crystal (randomly textured photonic crystal;
RTPC). The influence of the texture on the optical performance of RTPCs is discussed using the results of
an experiment and a finite-difference time-domain simulation. This RTPC back reflector (BR) can provide
high reflectivity and strong light scattering, resulting in an increased photocurrent density of the
hydrogenated amorphous silicon (a-Si:H) solar cell. As a result, the highly textured RTPC BR yielded an
efficiency of 9.6% for a-Si:H solar cell, which is much higher than the efficiency of 7.6% on flat AZO/Ag BR
and 9.0% on textured AZO/Ag BR. This RTPC BR provides a new approach for creating high-efficiency, low-
cost thin-film silicon solar cells.
& 2015 Elsevier B.V. All rights reserved.
1. Introduction
Light trapping is well established as a technique for improving
the energy conversion efficiency in thin- film silicon solar cells [1–
4]. In thin-film silicon solar cells with a substrate configuration (n–
i–p structure; n-doped layer/intrinsic layer/p-doped layer), the
typical thickness of the indium tin oxide (ITO) front contact ranges
from 60 nm to 80 nm for a suitable anti-reflective quality [5–7].It
is difficult to produce a textured surface for additional light trap-
ping effect with such a thin ITO layer. Therefore, in n–i–p thin-film
silicon solar cells, light trapping is primarily caused by the tex-
tured back reflector (BR), which plays a more crucial role than in
their superstrate (p–i–n) counterparts [6,8]. The most widely used
BRs for high efficiency n–i–p thin-film silicon solar cells are com-
posed of aluminum-doped zinc oxide (AZO)/Ag with a randomly
textured surface, which can be produced by combining the BR
structure with a thermally roughened textured Ag [8,9] or a silver-
covered randomly textured substrate [10–12]. It is well known that
a larger-scale texture provides superior light trapping [10,13].
However, in traditional BRs, there is a trade-off between a suitable
light scattering texture and the losses due to surface plasmon
absorptions from the rough surface of the metallic layer [14–16].
Such losses are cumulative over each reflection on the active layer/
rough metallic interface and become severe at higher photon
wavelengths because multiple optical passes are required [17].In
addition, the cost reduction achieved through efficiency
enhancement using AZO/Ag BRs is partly counterweighed by the
expensive raw material, silver.
In the past decade, several advanced light trapping concepts
and structures, such as the three-dimensional photonic crystal
intermediate reflector [18], modulated surface textures [19], plas-
monic light trapping [20,21], periodic honeycomb pattern sub-
strates [22], and photonic design [23,24], have attracted much
interest for improving the performance of solar cells. A highly
promising alternative approach is to use a dielectric one-dimen-
sional photonic crystal (1D PC), which is a multilayer structure in
which two layers (bilayers) with a high refractive-index contrast
are periodically stacked [25,26]. The 1D PC has a wide forbidden
band with a range of several hundreds of nanometers with nearly
100% reflectivity, which guarantees that almost no light can
transmit through the backside [27–29]. So it can be used as a
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journal homepage: www.elsevier.com/locate/solmat
Solar Energy Materials & Solar Cells
http://dx.doi.org/10.1016/j.solmat.2015.06.050
0927-0248/& 2015 Elsevier B.V. All rights reserved.
n
Corresponding author. Tel.: þ 86 22 23508663.
E-mail addresses: gfhou@nankai.edu.cn (G. Hou),
jjzhang@nankai.edu.cn (J. Zhang).
Solar Energy Materials & Solar Cells 143 (2015) 435–441