Journal of Physics D: Applied Physics
J. Phys. D: Appl. Phys. 47 (2014) 394017 (8pp) doi:10.1088/0022-3727/47/39/394017
Characterization and analysis of InAs/p–Si
heterojunction nanowire-based solar cell
Anna Dalmau Mallorqu´ ı, Esther Alarc ´ on-Llad ´ o, Eleonora Russo-Averchi,
G¨ ozde T ¨ ut ¨ unc ¨ uoglu, Federico Matteini, Daniel R ¨ uffer and
Anna Fontcuberta i Morral
Laboratoire des Mat´ eriaux Semiconducteurs,
´
Ecole Polytechnique F´ ed´ erale de Lausanne,
1015 Lausanne, Switzerland
E-mail: anna.dalmaumallorqui@epfl.ch and anna.fontcuberta-morral@epfl.ch
Received 12 March 2014, revised 26 April 2014
Accepted for publication 2 May 2014
Published 11 September 2014
Abstract
The growth of compound semiconductor nanowires on the silicon platform has opened many
new perspectives in the area of electronics, optoelectronics and photovoltaics. We have grown
a1 × 1 mm
2
array of InAs nanowires on p-type silicon for the fabrication of a solar cell. Even
though the nanowires are spaced by a distance of 800 nm with a 3.3% filling volume, they
absorb most of the incoming light resulting in an efficiency of 1.4%. Due to the unfavourable
band alignment, carrier separation at the junction is poor. Photocurrent increases sharply at the
surrounding edge with the silicon, where the nanowires do not absorb anymore. This is further
proof of the enhanced absorption of semiconductors in nanowire form. This work brings
further elements in the design of nanowire-based solar cells.
Keywords: InAs, molecular beam epitaxy, solar cell, light absorption
(Some figures may appear in colour only in the online journal)
1. Introduction
Compound semiconductors (III–V) are of special interest for
electronic and optoelectronic devices thanks to their high
electron mobility and direct band gap [1–3]. A key issue
to make them attractive for industrial applications is their
integration on the widely developed Si platform. There are
numerous challenges for a successful integration of III–Vs
on silicon, such as lattice mismatch, differences in thermal
expansion coefficients and polarity [4]. It has been shown that
III–V nanowires can overcome these challenges thanks to their
small footprint [5–7]. In the case of nanowires the strain can be
relaxed laterally thanks to their small diameter and dislocations
are present only at the interface, with little impact on the device
performance [8, 9]. Alternative high potential devices consider
the heterojunction between Si and a monolayer semiconductor
such as graphene [10, 11] or MoS
2
[12, 13].
In numerous applications a control on the position and
orientation of the nanowires is required. Vertical orientation of
nanowires can be achieved on Si (1 1 1) substrates in very high
yields [14–16]. In the case of catalyst-free growth, ordered
arrays of nanowires can in principle be attained by employing
a patterned SiO
2
mask [15, 17–19].
Among the applications of III–V arrays on silicon
are tunnel diodes [23], photoelectrochemical water splitting
[24, 25] and solar cells [26, 27]. By combining a GaAs
nanowire array on a silicon cell, a dual junction with a
theoretical efficiency higher than 30% could, in theory, be
achieved [28]. Another consequence of the nanowire small
diameter is that light absorption can only be understood from
a wave optics perspective. This results in the appearance of
interesting phenomena such as the presence of guided and
leaky modes [29, 30]. Recently, it has been shown that standing
semiconductor nanowires are extremely efficient in absorbing
light [31–33]. Their absorption cross-section is much larger
than their physical bounds. Thanks to this property, the optimal
design of nanowire-based solar cells includes arrays with a
relatively large pitch, leading to very large void fractions up to
90%. This discovery has led to the achievement of InP solar
cells with an efficiency up to 13.8% [34]. The achievement
of such an efficiency by other groups is limited to the ability
of growing these high quality arrays and by the ability of
producing the devices with high yield. The challenges linked
to the growth of GaAs arrays on silicon have hampered so far
the achievement of a GaAs nanowire array solar cell on silicon
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