Growth and characterization of ZnO/ZnTe core/shell nanowire arrays on transparent conducting oxide glass substrates
© Lin et al.; licensee Springer. 2012
Received: 16 May 2012
Accepted: 17 July 2012
Published: 17 July 2012
We report the growth and characterization of ZnO/ZnTe core/shell nanowire arrays on indium tin oxide. Coating of the ZnTe layer on well-aligned vertical ZnO nanowires has been demonstrated by scanning electron microscope, tunneling electron microscope, X-ray diffraction pattern, photoluminescence, and transmission studies. The ZnO/ZnTe core/shell nanowire arrays were then used as the active layer and carrier transport medium to fabricate a photovoltaic device. The enhanced photocurrent and faster response observed in ZnO/ZnTe, together with the quenching of the UV emission in the PL spectra, indicate that carrier separation in this structure plays an important role in determining their optical response. The results also indicate that core/shell structures can be made into useful photovoltaic devices.
KeywordsZnO/ZnTe core/shell nanowire arrays indium tin oxide glass substrates
ZnO is a material with great potential for a wide variety of practical applications. ZnO has a bandgap of 3.37 eV at room temperature and is emerging as a potential alternative to GaN in optoelectronic application, including piezoelectric transducers, optical waveguides, and transparent conducting oxides . In addition, ZnO has a high exciton binding energy of 60 meV that makes it an ideal candidate for optical devices such as UV light-emitting diodes, UV lasers , and UV photodetectors. In the past decade, ZnO nanowire-based photovoltaic devices, such as ZnO single-nanowire photodetectors, which have a small volume, a small active region, and a high internal gain ; ZnO p-n junction nanowire photodetectors, which exhibit clear rectifying characteristics and good ultraviolet light absorption ; and ZnO nanowire-quantum dot photovoltaic devices which can increase the absorption region with different wavelengths , have been studied. Recently, type-II heterojunction core/shell nanowires [6–9] have attracted much attention because the band alignment of these structures can separate the electron and hole into different spatial regions and thus can increase the carrier lifetimes. Vertically aligned core/shell nanowire arrays with these kinds of band structure can find wide applications in optoelectronic devices such as solar cells because they have higher surface-to-volume ratio, better light-trapping effect, and longer carrier lifetime as compared to the planar structures .
Amongst the type-II core/shell structures, the ZnO-based nanowire array is of particular interest because ZnO has excellent chemical stability, high surface-to-volume ratio, high refractive index, is nontoxic, and is friendly to the environment. As a result, interesting results have been obtained in ZnO/ZnSe , ZnO/ZnS , and ZnO/CdTe [8, 9] nanowire arrays. On the other hand, the ZnO/ZnTe nanowire array is expected to be an ideal system for photovoltaic applications . First, as-grown ZnTe is usually a p-type material and as-grown ZnO is usually n-type; therefore, n-ZnO/p-ZnTe heterostructure nanowires such as nano-p-n junctions and photodiodes may be readily fabricated. Second, like ZnO, ZnTe is nontoxic and is thus environment-friendly. Most importantly, the bandgap of bulk ZnTe is 2.34 eV, which is considerably smaller than that of ZnO and can greatly enhance absorption in the visible spectrum. Given the present intense interest in core/shell photodiodes  and one-dimensional nanostructures , it is therefore highly desirable to prepare and investigate ZnO/ZnTe nanowire arrays. However, to date, there seems to be a dearth of study of ZnO/ZnTe core/shell nanowire arrays, and it is the purpose of this letter to report the successful growth of such a structure. It is found that ZnTe can be coated on ZnO nanowires as supported by scanning electron microscope (SEM), transmission electron microscope (TEM), X-ray diffraction (XRD) pattern, photoluminescence (PL), and transmission studies. We also show that our ZnO/ZnTe core/shell array can have good optical properties and may find applications as a photovoltaic device.
We now describe the fabrication process of our ZnO/ZnTe core/shell array. Indium tin oxide (ITO) glass substrates, with a thickness of 135 nm and an electrical resistivity of 15 Ω/sq, were chosen to be used as transparent conducting oxide glass substrates because of their optical transparency and high electrical conductivity. The ITO glass substrate was then cut into 10 mm × 20 mm pieces. We note that it is important to clean the substrate thoroughly so as to achieve successful growth of our devices. To this end, the ITO glass substrate was cleaned ultrasonically in acetone, ethanol, and deionized water. Finally, the substrates were dried and cleaned by blowing dry nitrogen gas. High-density ZnO nanowire arrays with low defect concentrations can now be directly grown on ITO glass substrates under catalyst-free and low-temperature conditions by chemical vapor deposition (CVD). About 0.5 g of zinc powders was put on the alumina boat, and the clean ITO glass substrate was placed at 2 cm downstream to zinc powders on the same alumina boat. Then, the alumina boat was inserted into the center of the quartz tube in the furnace to grow ZnO nanowire arrays. The furnace was heated under a constant flow of 37 sccm Ar and 5 sccm O2 to 600°C for the growth of ZnO nanowire arrays. This reaction at 600°C reacted for 40 min, and then the furnace was turned off. The furnace was allowed to cool down to room temperature. In this way, ZnO nanowire arrays were successfully grown on the ITO glass substrate . The ZnO nanowire arrays on the ITO glass substrate were transferred into the metal oxide chemical vapor deposition (MOCVD) chamber to deposit the ZnTe shell for 700 s at 550°C and 760 Torr. Nitrogen was the carrier gas for the precursor combination dimethylzinc (DMZn) and dimethyl telluride (DMTe). It was essential to control the flow rate precisely because the ZnTe shell was just only tens of nanometer. The optimal flow rate of DMZn and DMTe was chosen to be 1:2 to flow through the MOCVD chamber by MFC .
Results and discussion
The bottom inset of Figure 4 shows the PL spectra of ZnO and ZnO/ZnTe core/shell nanowire arrays measured at room temperature. The PL peak near the band edge of ZnO is found to be very strong with negligible emission peaks associated with deep-level defects. Compared with that of the bare ZnO nanowire arrays, the peak position of the UV emission in ZnO/ZnTe core/shell nanowire arrays shows a small blueshift, and the intensity is reduced by a factor of 850. This result also indicates that the charge carrier separation driven by the type-II band alignment between ZnO and ZnTe serves as the major contributor to the quenching of the PL peak at 384 nm near the band edge of ZnO, while interfacial recombination, depletion, and photon blocking have little contributions.
Figure 4 shows the transmission spectra of ZnO/ZnTe core/shell nanowire arrays. There are two abrupt drops near 390 and 550 nm in the transmission curve, corresponding well to the bandgap of ZnO and ZnTe, respectively. The transmission intensity of ZnO/ZnTe core/shell nanowire arrays not only increases at 390 and 550 nm but also increases gradually in other regions. The component in other regions can raise from a spatially indirect or an interfacial transition, coupling a hole state in the ZnTe shell with an electron state in the ZnO core.
In summary, well-aligned ZnO/ZnTe core/shell nanowire arrays were successfully fabricated on transparent conducting oxide glass substrates by CVD and MOCVD. The structures' properties were investigated in detail by SEM, TEM, and XRD studies; the results showed the core/shell structure that the ZnTe shell deposited directly in the radial direction from the surface of the ZnO nanowire. The ZnO core was consisted of the (002) plane of wurtzite structure; the ZnTe shell was consisted of the (111) plane of zincblende structure. The optical properties were investigated by PL and transmission studies. The results showed that the ZnO/ZnTe core/shell nanowires have desirable optical properties. The ZnO/ZnTe core/shell nanowire arrays were then used as the active layer and carrier transport medium to fabricate a photovoltaic device. The enhanced photocurrent and faster response observed in ZnO/ZnTe, together with the quenching of the UV emission in the PL spectra, indicate that carrier separation in this structure plays an important role in determining their optical response. The results also indicate that core/shell structures can be made into useful photovoltaic devices.
YWL obtained his M.Sc. degree at National Taiwan University (NTU). WJC obtained his M.Sc. degree at NTU and is currently a Ph.D. student working at the Department of Physics, NTU. JYL obtained his Ph.D. degree at NTU and is currently an engineer working for TSMC, Taiwan. YHC obtained his B.Sc. degree at National Tsing Hua University, Taiwan and his Ph.D. degree at the University at Buffalo, USA, and is currently the Director of the Science and Technology Division, Taipei Economic and Cultural Center in India and a professor of Physics, NTU. CTL obtained his B.Sc. degree at NTU in 1990 and his Ph.D. degree in Physics at Cambridge University, UK in 1996 and is currently a professor of Physics at NTU. YFC obtained his B.Sc. degree at National Tsing Hua University, Taiwan and his Ph.D. degree at Purdue University, USA, and is currently a chair professor at NTU. JYL obtained his B.Sc. degree at Fu Jen Catholic University, Taiwan, and his M.Sc. degree at Tamkang University, Taiwan, and is currently a technician in charge of the TEM facility, NTU.
chemical vapor deposition
indium tin oxide
metal oxide chemical vapor deposition
scanning electron microscope
transmission electron microscope
This work was supported by the National Science Council of the Republic of China under contract no. NSC 100-2112-M-002-017-MY3. CTL thanks Tina Liang, Valen Liang, and Eva Liang for their support.
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