Surface photovoltage investigation of recombination at the a-Si/c-Si heterojunction
L. Korte
a,
⁎, A. Laades
a,b
, K. Lauer
b,c
, R. Stangl
a
, D. Schaffarzik
a
, M. Schmidt
a
a
Helmholtz-Zentrum Berlin für Materialien und Energie, Abteilung Silizium-Photovoltaik, Kekuléstr.5, D-12489 Berlin, Germany
b
CiS Institut für Mikrosensorik GmbH, SolarZentrum Erfurt, Konrad-Zuse-Str. 14, D-99099 Erfurt, Germany
c
TU Ilmenau, Institut für Physik, Weimarer Str. 32, 98693 Ilmenau, Germany
abstract article info
Available online 21 February 2009
Keywords:
Surface photovoltage
Band bending
Interface defects
Amorphous/crystalline heterojunction
We investigate the use of time-resolved surface photovoltage (SPV) transients as a means to determine band
bending and recombination properties at amorphous/crystalline silicon (a-Si:H/c-Si) heterojunctions.
Experimentally, it is shown that for a-Si:H film thicknesses above ~6 nm, SPV transients do not depend on
the film thickness anymore. On this basis, a simple numerical model is proposed that consists of a single
rechargeable gap state on the c-Si wafer surface, into which the properties of the a-Si:H/c-Si interface and
the adjacent a-Si:H are lumped. It is shown that this model can reproduce all principal features of high
excitation SPV transients, i.e. an initial fast decay shown to be due to Auger recombination, a plateau region
for high injection conditions and a fast decay when the sample returns into low injection and the defect
states are recharged. Under sufficiently high excitation, the SPV saturates at a value that is determined by the
a-Si:H/c-Si interface band bending in the dark. From the slope of the transient decay, defect parameters
(density, energetic position) can be extracted.
© 2009 Elsevier B.V. All rights reserved.
1. Introduction
Amorphous/crystalline silicon heterojunctions produced by
plasma enhanced chemical vapour deposition (PECVD) of ultrathin
(5–10 nm) hydrogenated amorphous silicon layers, a-Si:H, on crys-
talline silicon substrates, c-Si, are an interesting concept for high-
efficiency solar cells on monocrystalline wafers, and to realize large
area heterojunction cell concepts on for low-cost thin-film silicon. For
those cell types, in order to achieve high efficiencies, it is necessary to
suppress interface recombination at the a-Si:H/c-Si interface. We
have shown previously [1], that this can be achieved by decreasing
the density of interface defect states D
it
(E) of the a-Si:H/c-Si inter-
face and/or by increasing the c-Si band bending qφ
s0
. Low D
it
can be
obtained by reducing the c-Si surface defect density prior to a-Si:H
deposition, and by choosing optimized a-Si:H deposition conditions
[2], while the band bending is adjusted by the a-Si:H doping. The a-Si:H
doping level has to be chosen as a trade-off between high band
bending and high density of a-Si:H gap states at increased doping
levels, which lead to enhanced recombination in the a-Si:H [3]. All
those optimizations profit greatly from a tool to characterize the
a-Si:H/c-Si interface recombination. To this end, we have been using
surface photovoltage measurements (SPV), especially in the time-
dependent and intensity-dependent modes (TD-SPV/ID-SPV) [4,5]
and references therein], as a “fingerprinting” method to monitor the
electronic properties of the a-Si:H/c-Si effective interface. With the
present paper, using numerical simulations, we aim at a refined
understanding of the mechanisms that determine the transient
decrease of photovoltage over time after the short illumination light
pulse. This will allow to extract a-Si:H/c-Si interface recombination
properties that can be compared, for adequate sample structures, to
those obtained by other means such as quasi-steady state and
microwave photoconductance decay (QSSPC and μPCD).
2. Sample preparation
Phosphorous-doped n-type amorphous silicon (a-Si:H) layers
were deposited by PECVD (base pressure 10
−7
mbar) on high quality
p-doped (resistivity 1–3 Ω cm) monocrystalline Si (c-Si) wafers with
b111N surface orientation and bulk diffusion lengths of several
100 μm. For experimental details, see e.g. [3,4]. a-Si:H/c-Si solar
cells produced using the same PECVD system have yielded maximum
efficiencies of 19.8% [6]. The investigated set of samples consists of
(n
+
)a-Si:H/(p)c-Si (a-Si:H doping 10
3
ppm PH
3
in the gas phase) with
increasing a-Si:H layer thickness (0.4 – 120 nm).
3. Experimental methods
3.1. Surface photovoltage
Surface photovoltage (SPV) is an electrical characterization
technique that is well-established for the determination of the density
of surface states especially at the silicon/silicon oxide interface [7].
The principle is described elsewhere [4,8] and will be briefly outlined
here: The sample under test is sandwiched in a structure consisting of
a transparent conductive front contact (TCO — typically zinc oxide), an
Thin Solid Films 517 (2009) 6396–6400
⁎ Corresponding author. Tel.: +49 30 80621351.
E-mail address: korte@helmholtz-berlin.de (L. Korte).
0040-6090/$ – see front matter © 2009 Elsevier B.V. All rights reserved.
doi:10.1016/j.tsf.2009.02.090
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