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Nanowire solar cells for next-generation photovoltaics

Nanowire components with the superior photovoltaic properties of III-V semiconductors can boost solar cell efficiency.
28 August 2013, SPIE Newsroom. DOI: 10.1117/2.1201308.005048

Current solar cell technologies are dominated by silicon. Limited primarily by silicon's inherent properties, these solar cells convert only 15–20% of solar energy into electricity. Solar cells made from III-V compound semiconductors (materials that contain group III and group V elements) have much higher efficiencies, due to their better optical (absorption) and electrical (charge mobility) properties. Furthermore, with different III-V materials on the same device, researchers can produce multiple junctions or heterostructures to cover a broader range of the solar spectrum. In these devices, researchers have demonstrated efficiencies of over 40% under concentrated solar energy.1

The additional benefits afforded by nanotechnology may further enhance solar cell performance. Nanowire research has emerged as a quickly growing field. Much excitement stems from the unique electronic and optical properties of semiconductor nanowires. Nanowires of a particular substance may behave quite unlike much larger ‘bulk’ samples of the same material. Nanowires are of great interest in photovoltaics because of their large surface area, high aspect ratio (long and thin), intrinsic antireflection effect (which increases light absorption), and ability to direct light absorption with specifically designed arrays.2

More importantly, core-shell nanowires, which operate based on radial p-n junctions, represent a revolution in photovoltaics by decoupling light absorption from carrier collection pathways: light is absorbed vertically, whereas carriers are separated radially. This separation eliminates the once-fundamental trade-off between light absorption and carrier collection. By incorporating the superior photovoltaic properties of III-V semiconductors into nanowire structures, researchers expect to achieve efficiencies similar to today's best solar cells, with significantly less material. Because nanowire-based cells use less material than planar devices, such changes can ultimately reduce costs.

Figure 1. Scanning electron microscopy (SEM) image of gallium arsenide/aluminum gallium arsenide (GaAs/AlGaAs) core-shell nanowires.

Figure 1 shows a scanning electron microscopy image of typical gallium arsenide/aluminum gallium arsenide (GaAs/ AlGaAs) core-shell nanowires used to fabricate solar cells. These nanowires are synthesized on GaAs platforms using the vapor-liquid-solid process—a technique that relies on gold nanoparticles to catalyze nanowire growth—in a metal organic chemical vapor deposition system. By optimizing growth conditions, we have significantly improved the crystal quality of the GaAs nanowires.3Furthermore, by growing a high-quality AlGaAs shell surrounding the GaAs nanowire, we achieved excellent optical quality and long carrier lifetimes.4 These properties are very desirable for solar cells because carriers can otherwise recombine easily at the surface and reduce the output current.

Figure 2. Left: Schematic diagram of a nanowire solar cell. Right: SEM image of BCB planarized nanowires peeled off from the substrate. Ti: Titanium. Au: Gold. BCB: Benzocyclobutene. ITO: Indium tin oxide. p, n, n+, n- : Different types of semiconductor materials. (111) refers to the crystal orientation of the substrate.

Since nanowires are non-planar structures, fabrication of nanowire devices requires non-standard semiconductor manufacturing processes. Figure 2(a) shows a schematic diagram of a prototype core-shell GaAs/AlGaAs nanowire solar cell and the necessary fabrication processes. The p-type semiconductor GaAs substrate and the n-type GaAs nanowires form a substrate-nanowire p-n junction device. Benzocyclobutene (BCB) resist, applied via spin coating and thermal curing, planarizes the vertically standing nanowires on the substrate. We chose BCB for its excellent planarizing characteristics, such as uniform coverage, and its excellent transmission and insulating properties. Inductively coupled plasma reactive ion etching with a sulfur hexafluoride and oxygen (SF6/O2) gas mixture then etches back the BCB to expose the nanowire tips for top contacts. Finally, sputtering and electron beam evaporation form a 200nm-thick transparent indium tin oxide layer and a titanium/gold (10nm/200nm) layer, as top n- and bottom p-contacts, respectively.

We measured good power conversion efficiency of 3.56% in these initial nanowire devices. With further optimization of nanowire geometry, growth, and processing procedures, we expect that the efficiency will improve significantly. We also found that we could peel off some of the underlying wafer, leaving a ribbon of nanowires securely embedded in the polymer layer: see Figure 2(b). This technique holds great promise for creating flexible and lightweight nanowire solar cells. Reduced material usage and substrate re-use should also help to lower costs. Such solar cells could be integrated into, rather than installed on, surfaces such as clothes and fabrics.

Figure 3. Photocurrent map along the growth direction of a single GaAs/AlGaAs nanowire, using the TOBIC (two-photon induced current) technique. Photocurrent generated from both a nanowire and the substrate below it can be clearly identified for in-depth study of carrier generation and collection.

To understand what is happening within the nanowire solar cells, we developed a novel technique based on two-photon induced current. The technique provides a 3D map of the photocurrent from each nanowire at submicrometer resolution.5Using ‘below bandgap’ (two-photon) laser excitation, carriers can be generated specifically at the focal voxel and not above or below this point within the focus cone (as would occur for above-gap excitation). Figure 3 shows photocurrent mapping along the growth direction of a single nanowire from our solar cell, revealing efficiency hotspots, carrier collection pathways, and recombination mechanisms with high spatial resolution. This technique opens up enormous opportunity to explore various nanowire solar cell designs and further exploit the unique properties of 1D nanostructures in high-efficiency photovoltaic devices. Nanowire solar cells show great promise for next-generation photovoltaics. However, addressing the many new material and device challenges that arise from these unconventional nanostructures will require more mature simulation, manufacturing, and characterization tools. Researchers must focus their attention on these goals to achieve high-performance devices that will find application in daily life.

This research is supported by the Australian Research Council, and facilities used in this work are supported by the Australian National Fabrication Facility. The processing expertise of Fouad Karouta and Kaushal Vora is gratefully acknowledged.

Yu-Heng Lee, Lan Fu, Zhe Li, Steffen Breuer, Hoe Tan, Chennupati Jagadish
The Australian National University
Canberra, Australia
Patrick Parkinson
University of Oxford
Oxford, United Kingdom

1. M. A. Green, K. Emery, Y. Hishikawa, W. Warta, E. D. Dunlop, Solar cell efficiency tables (version 41), Prog. Photovolt.: Res. Appl. 21, p. 1-11, 2013.
2. J. Wallentin, N. Anttu, D. Asoli, M. Huffman, I. Aberg, M. H. Magnusson, G. Siefer, P. Fuss-Kailuweit, InP nanowire array solar cells achieving 13.8% efficiency by exceeding the ray optics limit, Science 339, p. 1057-1060, 2013.
3. H. J. Joyce, Q. Gao, H. H. Tan, C. Jagadish, Y. Kim, X. Zhang, Y. Guo, J. Zou, Twin-free uniform epitaxial GaAs nanowires grown by a two-temperature process, Nano Lett. 7, p. 921-926, 2007.
4. N. Jiang, P. Parkinson, Q. Gao, H. H. Tan, Y. Wong-Leung, C. Jagadish, Long minority carrier lifetime in Au-catalyzed GaAs/AlxGa1-xAs core-shell nanowires, Appl. Phys. Lett. 101, p. 023111, 2012.
5. P. Parkinson, Y.-H. Lee, L. Fu, S. Breuer, H. H. Tan, C. Jagadish, Three-dimensional in situ photocurrent mapping for nanowire photovoltaics, Nano Lett. 13, p. 1405-1409, 2013.