- Nano Express
- Open Access
Formation of Nb2O5 matrix and Vis-NIR absorption in Nb-Ge-O thin film
Nanoscale Research Letters volume 7, Article number: 341 (2012)
This paper investigates the crystal structure and optical absorption of Ge-doped Nb-oxide (Nb-Ge-O) thin films prepared by RF sputtering. A wide-gap material, Nb2O5, is selectively produced as a matrix to disperse Ge nanocrystals through compositional optimization with Ge chip numbers and oxygen ratio in argon. The optical-absorption spectra are obviously shifted to visible (vis) and near-infrared (NIR) regions, suggesting that a composite thin film with Ge nanocrystals dispersed in Nb2O5 matrix exhibits quantum-size effects. Accordingly, the two valuable characteristics of the Nb2O5 matrix and the vis-NIR absorption are found to be retained simultaneously in Nb-Ge-O thin films.
Quantum-dot solar cells have attracted much attention because of their potential to increase conversion efficiency . Specifically, the optical-absorption edge of a semiconductor nanocrystal is often shifted due to the quantum-size effect. The optical band gap can then be tuned to the effective energy region for absorbing the maximum intensity of the solar radiation spectrum. Furthermore, quantum dots produce multiple electron–hole pairs per photon through impact ionization, whereas bulk semiconductor produces one electron–hole pair per photon.
A wide-gap semiconductor sensitized by semiconductor nanocrystals is a candidate material for such use. Wide-gap materials such as TiO2 and ZnO can only absorb the ultraviolet (UV) part of the solar radiation spectrum. Hence, the semiconductor nanocrystal supports the absorption of visible (vis) and near-infrared (NIR) light. Up to now, various nanocrystalline materials (InP , CdSe , CdS [4, 5], PbS , and Ge [7, 8]) have been investigated as sensitizers for TiO2. Alternatively, the wide-gap semiconductor ZnO was also investigated, since the band gap and the energetic position of the valence band maximum and conduction band minimum of ZnO are very close to that of TiO2. Most of these composite materials were synthesized through chemical techniques, although physical deposition, such as sputtering, is also useful. In addition, package synthesis of composite thin film is favorable for low-cost production of solar cells. Package synthesis requires a specific material design for each deposition technique, for example radio frequency (RF) sputtering  and hot-wall deposition . The present study proposes a new composite thin film with Ge nanocrystals dispersed in Nb2O5 matrix by RF sputtering. According to the material design, based on differences in the heat of formation , Ge nanocrystals are thermodynamically stable in an Nb2O5 matrix, since Nb is oxidized more than Ge because the heat of formation of GeO2 exceeds that of Nb2O5. In addition, nanocrystalline Ge dispersed in the Nb2O5 matrix may exhibit quantum-size effects due to the wide band gap of 3.4 eV in Nb2O5. However, it is difficult to forecast how Nb oxides (typically NbO, NbO2, and Nb2O5) will be formed during the preparation process. Among these compounds, only Nb2O5 satisfies the present objective. In the current study, the composition of Ge-doped Nb-oxide (Nb-Ge-O) thin film is varied widely to produce single-phase Nb2O5 as the matrix, while retaining vis-NIR absorption due to the presence of Ge nanocrystals.
An Nb-Ge-O thin film was prepared by RF sputtering from a composite target. Specifically, 5 × 5 mm2 Ge-chips were set on a 4-in.-diameter ceramic Nb2O5 target. The chamber was first evacuated to a vacuum of 1.5 × 10−7 Torr, and the thin film was deposited on a Corning #7059 glass substrate cooled by water. The substrate was cleaned with an acetone ultrasonic bath for 60 min to remove surface contaminations, dried using nitrogen air gun, and finally sputter-etched at an applied power of 200 W for 1 min. The distance between the target and the substrate was kept constant at 73 mm. The total gas pressure of argon or argon and additional oxygen was fixed at 2.0 × 10−3 Torr. RF power and deposition time were kept constant at 200 W and 90 min, and no RF bias was applied to the substrate. The Nb-Ge-O thin films thus deposited were successively post-annealed at 923 K for 60 min in a vacuum to crystallize Ge nanocrystals and the Nb-O matrix. The Nb-Ge-O thin film was structurally characterized using X-ray diffraction (XRD, Rigaku RAD-X, Rigaku Corporation, Tokyo, Japan) with Cu Kα radiation. The optical-absorption spectrum of the film was measured using UV–vis-NIR spectroscopy (Shimadzu UV5300, Shimadzu Corporation, Nakagyo-ku, Kyoto, Japan), and the composition of the film was analyzed using energy-dispersion spectroscopy (EDAX Phoenix, NJ, USA), operating at 10 kV with standard samples of KNbO3 to calibrate the analyzed results for elements Nb and O, and with Bi4Ge3O12 for element Ge. Nanoscale elemental mapping was performed using scanning transmission electron microscopy (STEM, Hitachi HD-2700, Hitachi, Ltd., Tokyo Japan) in EDX mode (EDAX model: Genesis) operating at 200 kV with an energy resolution of 150 eV. Ion milling was performed during sample preparation.
Results and discussion
Figure 1 presents the XRD pattern of the Nb-Ge-O thin films prepared in a pure Ar atmosphere. The as-deposited films formed an amorphous structure, and post-annealing was therefore performed to crystallize both Ge and Nb-oxide. Regarding temperature variations in a preliminary experiment (not shown here), XRD peaks of both Ge and Nb-oxide appeared at 823 K, and the peak of Ge became more prominent at 923 K. Thus, a post-annealing temperature of 923 K is employed here. At Ge = 0 at.%, a phase mixture of NbO2 and Nb2O5 with an orthorhombic structure is observed. The peak of NbO2 with a tetragonal structure disappears at a Ge concentration of 1.8 at.%, and the XRD peak of Ge appears instead. Further addition of Ge exceeding 4.9 at.% reproduces the weak NbO2 peak. Figure 2 presents the optical transmittance and reflectance spectra of the Nb-Ge-O thin films. The optical absorption edge of the Nb2O5 is clearly seen at 0 at.%, with relatively less transparency in the vis-IR range. This transparency is favorably improved at 1.8 at.% Ge, but further additions (4.9 at.% and 5.5 at.%) also reduce the transparency. The reflectance spectra exhibit no significant difference in vis-NIR range. Scanning electron microscopy also revealed a relatively flat appearance irrespective of the Ge concentration (not shown here). In addition, the thickness of the films increase gradually from 1,200 nm (0 at.% Ge) to 1,600 nm (5.5 at.% Ge) with increasing Ge composition. Thus, the relatively low transparency in vis-NIR range at 0 at.% and 5.5 at.% is not due to surface morphology and thicker nature. In contrast, the optical absorption edge monotonically shifts toward the long-wavelength region as the Ge concentration increases. The addition of Ge to Nb-oxide thus induces a transparency change and an absorption shift. Figure 3 plots the XRD peak intensity ratio of NbO2 at (400) reflection and Nb2O5 at (001) reflection, and the optical transparency at 1,000 nm for the Nb-Ge-O thin films. The XRD intensity ratio is minimized at 1.8 at.% Ge, with a maximum transparency at 1,000 nm. Hence, the transparency increases with decreasing NbO2 phase. In a preliminary experiment with diffused reflectance spectra, a standard powder of NbO2 exhibited opacity over a wide range from UV to NIR, in contrast with the visible transparency of Nb2O5. Thus, the change in the optical transparency (Figure 2) is due to the inclusion of NbO2.
The relation between the analyzed composition of the films and the structure derived from the XRD pattern is summarized in Figure 4. The stoichiometric composition of Nb2O5 is presented as a dotted line. The squares indicate the phase mixture of Nb2O5 and GeO2, which appears in a relatively high oxygen concentration range beyond the stoichiometry line of Nb2O5. In this case, the added Ge is fully oxidized, with no optical absorption shift toward the vis-NIR region. The triangles indicate the phase mixture of Nb2O5 and NbO2, which appears together with Ge phase in relatively high-Ge compositions and also appears in pure Nb-oxide (i.e., no Ge) in relatively lower-oxygen compositions. The black dots indicate the single phase Nb2O5, which appears in relatively low Ge compositions. The red dots indicate a phase mixture of Ge and Nb2O5, which appears in a quite narrow range of Ge concentration from 1.0 at.% to 1.8 at.%, near the stoichiometry line. The crystal structure of the Nb-Ge-O films thus changes, and single-phase Nb2O5 is selectively produced as a result of compositional optimization.
Figure 5 presents typical optical absorption spectra for the Nb-Ge-O thin films with a phase mixture of Ge and Nb2O5. For comparison, the spectrum of a pure Nb2O5 thin film (A), and phase mixture of Ge, Nb2O5, and NbO2 (D) are also presented in the figure. An intact absorbance is employed here to exactly evaluate the absorption edge. At 0 at.% Ge, the optical absorption edge of Nb2O5 is clearly observed at 3.4 eV. The broad absorption edge shifts toward the lower-energy region as the Ge content increases. In particular, onset absorption can be confirmed at 1.0 eV with 1.5 at.% Ge, favorably covering the desirable energy region for high conversion efficiency . Therefore, it should be noted that the Nb-Ge-O thin film exhibits the valuable characteristic of vis-NIR absorption.
There are two possible reasons for the shift in the optical absorption edge, forming a solid solution matrix of (Nb2O5)1−x(GeO2) x and exhibiting the quantum-size effect in Ge nanocrystals. The solid solution of (Nb2O5)1−x(GeO2) x was investigated first. Nb-Ge-O thin film often contains multiple phases, and it is then difficult to focus on the matrix characteristics. The (Nb2O5)1−x(GeO2) x solid solution is therefore powder-synthesized here. This system was found to form a solid solution [15, 16], but the energy band gap of this system is still unclear. The fundamental properties of the solubility range of Ge and the energy band gap were therefore investigated to clarify whether the ternary solid solution exhibits vis-NIR absorption. Figure 6 presents the powder XRD pattern of the (Nb2O5)1−x(GeO2) x system. In the powder synthesis, standard powders of orthorhombic Nb2O5 (3 N pure) and GeO2 (4 N pure) were used as a starting materials. The powders were weighed for the desired composition, mixed in an agate mortar, and pressed at 49 MPa to promote a solid-state reaction. Heat treatment was performed at 1,273 K for 96 h in air to achieve thermal equilibrium, followed by water-quenching to maintain the solubility range at the synthesis temperature. The sample, thus heat-treated, was well hardened and then crushed into powder for the following experiment setup. The composition of the (Nb2O5)1−x(GeO2) x system, thus powder-synthesized, is the nominal value. In the preliminary experiment, a mass reduction during the heat treatment was found to be less than 1% in standard powders of Nb2O5 and GeO2, suggesting a quite small amount of sublimation. The nominal content of Ge is therefore employed here as a composition of the production. At x = 0, all of the XRD peaks are assigned to the monoclinic Nb2O5. The XRD peak of GeO2 appears at x = 0.18, forming a phase mixture of GeO2 and Nb2O5. It is suggested that the present sample possibly forms a solid solution of (Nb2O5)1-x(GeO2) x at compositions below x = 0.18.
Next, the solubility limit of Ge in Nb2O5 is determined through variations in the lattice constant. Figure 7 plots the lattice constant of the (Nb2O5)1−x(GeO2) x solid solution as a function of x. Here, the lattice constant of the orthorhombic system is estimated from the (005) and (020) reflections. It is clearly seen in the figure that the lattice constant first increases linearly in proportion to x and then becomes nearly constant irrespective of x in the range exceeding 0.14 in both the (005) and (020) reflections. According to Vegard's law , an on-setting composition x deviating from linearity is regarded as the solubility limit of GeO2 in Nb2O5. This was therefore determined to be 0.14 at 1,273 K. This result strongly suggests that the Nb2O5 phase in the Nb-Ge-O thin film (Figure 4) may have formed a solid solution of (Nb2O5)1−x(GeO2) x . Subsequently, optical absorption of the (Nb2O5)1−x(GeO2) x thus powder-synthesized should be investigated regardless of whether the solid solution exhibits vis-NIR absorption.
Figure 8 plots the optical absorption spectra of the powder-synthesized (Nb2O5)1−x(GeO2) x solid solution. These spectra are derived from the Kubelka-Munk function . For comparison, the spectrum of orthorhombic Nb2O5 and GeO2 is also shown. It is clearly seen that the GeO2 is fully transparent over the measured range from 2.7 to 4.5 eV, whereas the optical absorption edge of the monoclinic (Nb2O5)1−x(GeO2) x can be clearly observed at 3.1 eV at x = 0 and shifts toward the higher-energy region as x increases. In addition, the band gap of orthorhombic Nb2O5 is higher than that of monoclinic Nb2O5. From these results, orthorhombic Nb2O5-phase in the Nb-Ge-O thin films may have formed a solid solution of (Nb2O5)1−x(GeO2) x during post-annealing at 923 K but did not exhibit vis-NIR absorption. The quantum-size effect in the Ge nanocrystals was also investigated as another possible reason for the absorption shift (Figure 5).
Figure 9a presents an image resulting from high-angle annular dark-field scanning transmission microscopy (HAADF-STEM) of the Nb-Ge-O thin film with a phase mixture of Ge and Nb2O5, containing 1.5 at.% Ge. In this case, Nb-oxide is compositionally optimized to form a single phase Nb2O5. The difference in atomic number can be determined by the observed contrast in the HAADF-STEM image. Several black grains are seen in the image in Figure 9a, but this black contrast is not due to the difference in atomic number, since there is no compositional change near the black grains on the STEM-EDX elemental mapping of the sample, based on X-ray detection of Nb L (blue) (Figure 9d) and O K (green) (Figure 9f). Hence, these black grains probably indicate a structural defect in the film. In another area with a gray color (Figure 9a), the graphic contrast is too weak to determine the difference in atomic number. The image contrast is thus emphasized in the enlarged Figure 9b for easier viewing. Gourd-shaped grains, which are schematically illustrated in Figure 9c, can be seen in the image. The gourd-shaped grains mainly indicate the absence of elemental Nb and O (Figures 9d,f) and the presence of Ge [Ge K (yellow), Figure 9e. It is thus determined that the gourd-shaped grains (Figure 9b) are dominantly nanocrystalline Ge. The other region is widely covered with the elements Nb and O (Figures 9d,f), reasonably assumed to form Nb-oxide. It is therefore determined that isolated Ge nanocrystals are dispersed in the Nb2O5 matrix. The mean grain size of the Ge nanocrystals is estimated to be 11 nm, according to the XRD result using Scherrer's equation . This is too small to exhibit the quantum-size effect because of the exciton Bohr radius of 24.3 nm in Ge . Assuming an infinite potential barrier, optical gap of the Ge nanocrystals with the mean size of 11 nm is calculated to be 1.1 eV using Brus model . This value is close to the onset absorption of 1.0 eV at 1.5 at.% Ge (Figure 5). Ge nanocrystals embedded in silica matrix also exhibits similar optical absorption spectrum, with the mean size of 6.0 nm estimated from direct observation using high-resolution transmission microscopy . Consequently, the shift of the optical absorption edge (Figure 5) is reasonably due to the presence of Ge nanocrystals embedded in the Nb2O5 matrix.
These results indicate that the Nb-Ge-O thin films can selectively produce the Nb2O5 matrix and the vis-NIR absorption simultaneously, despite the package synthesis by RF sputtering. One-step synthesis of a composite package with Ge nanocrystals dispersed in Nb2O5 matrix therefore has the potential to yield low-cost production of next-generation solar cells.
A new composite thin film with Ge nanocrystals dispersed in Nb2O5 matrix has been proposed as a candidate material for quantum-dot solar cells. It should be pointed out that single-phase Nb2O5 appears in a restricted composition range from 1.0 to 1.8 at.% Ge as a result of compositional optimization based on the Ge chip number and oxygen ratio in argon. Furthermore, the optical absorption edge shifts toward the lower-photon-energy region as the Ge content increases. In particular, onset absorption can be confirmed at 1.0 eV with 1.5 at.% Ge, favorably covering the desirable energy region for high conversion efficiency. Elemental mapping indicates that the isolated Ge nanocrystals are dispersed in the Nb2O5 matrix. Thus, two valuable characteristics, the selective production of Nb2O5 and vis-NIR absorption, are simultaneously retained in Nb-Ge-O thin films.
SA is a group leader of Research Institute for Electromagnetic Materials.
Nozik AJ: Quantum dot solar cells. Phys E 2002, 14: 115–120. 10.1016/S1386-9477(02)00374-0
Zaban A, Micic OI, Gregg BA, Nozik AJ: Photosensitization of nanoporus TiO2 electrodes with InP quantum dots. Langmuir 1998, 14: 3153–3156. 10.1021/la9713863
Liu D, Kamat PV: Photoelectrochemical behavior of thin CdSe and coupled TiO2/CdSe semiconductor films. J Phys Chem 1993, 97: 10769–10763. 10.1021/j100143a041
Weller H: Quantum sized semiconductor particles in solution in modified layers. Ber Bunsen-Ges Phys Chem 1991, 95: 1361–1365. 10.1002/bbpc.19910951108
Zhu G, Su F, Lv T, Pan L, Sun Z: Au nanoparticles as interfacial layer for CdS quantum dot-sensitized solar cells. Nanoscale Res Lett 2010, 5: 1749–1754. 10.1007/s11671-010-9705-z
Hoyer P, Könenkamp R: Photoconduction in porus TiO2 sensitized by PbS quantum dots. Appl Phys Lett 1995, 66: 349–351. 10.1063/1.114209
Chatterjee S, Goyal A, Shah I: Inorganic nanocomposites for next generation photovoltaics. Mater Lett 2006, 60: 3541–3543. 10.1016/j.matlet.2006.03.048
Abe S, Ohnuma M, Ping DH, Ohnuma S: Anatase-dominant matrix in Ge/TiO2 thin films prepared by RF sputtering method. Appl Phys Exp 2008, 1: 095001.
Yang W, Wan F, Chen S, Jiang C: Hydrothermal growth and application of ZnO nanowire films with ZnO and TiO2 buffer layers in dye-sensitized solar cells. Nanoscale Res Lett 2009, 4: 1486–1492. 10.1007/s11671-009-9425-4
Ohnuma S, Fujimori H, Mitani S, Masumoto T: High-frequency magnetic properties in metal-nonmetal granular films. J Appl Phys 1996, 79: 5130–5135. 10.1063/1.361531
Abe S: One-step synthesis of PbSe-ZnSe composite thin film. Nanoscale Research Letters 2011, 6: 324. 10.1186/1556-276X-6-324
Kubachevski O: Alcock CB: Metallurgical Thermochemistry. Pergamon, Oxford; 1979.
Yoshimura K, Miki T, Iwama S, Tanemura S: Characterization of niobium oxide electrochromic thin films prepared by reactive d. c. magnetron sputtering. Thin Solid Films 1989, 59: 172.
Loferski JJ: Theoretical considerations covering the choice of the optimum semiconductor for photovoltaic solar energy conversion. J Appl Phys 1956, 27: 777–784. 10.1063/1.1722483
Levin EM: Phase equilibria in the niobium pentoxide-germanium dioxide. J Res Nat Bur Stand 1966, 70A: 5–10.
Yamaguchi O, Mukaida Y: Formation of niobium germanate from Nb2O5 solid solution in the system Nb2O5-GeO2. Br Ceram Trans J 1989, 88: 91–94.
Vegard L: Die Konstitution der Mischkristalle und die Raumerfüllung der Atome. Z Phys 1921, 5: 17–26. 10.1007/BF01349680
Kubelka P, Munk F: Ein Beitrag zur Optik der Far-banstriche. Z Tech Phys 1931, 12: 593–601.
Scherrer P: Bestimmung der Größe und der inneren Struktur von Kolloidteilchen mittels Röntgenstrahlen. Göttinger Nachrichten 1918, 2: 98–100.
Maeda Y, Tsukamoto N, Yazawa Y, Kanemitsu Y, Masumoto Y: Visible photoluminescence of Ge microcrystals embedded in SiO2. Appl Phys Let 1991, 59: 3168–3170. 10.1063/1.105773
Brus LE: Zero-dimensional excitons in semiconductor clusters. IEEE J Quantum Electron 1986, 22: 1909–1914. 10.1109/JQE.1986.1073184
Giri PK, Kesavamoorthy R, Panigrahi BK, Nair GM: Evidence for fast decay dynamics of the photoluminescence from Ge nanocrystals embedded in SiO2. Sold State Comm 2005, 133: 229–234. 10.1016/j.ssc.2004.11.007
The present work was supported by a Grant-in-Aid for Scientific Research from the Japan Society for the Promotion of Science (No. 18360338). The author gratefully acknowledges the valuable comments and continuous encouragement of President T. Masumoto [Research Institute for Electromagnetic Materials (DENJIKEN), Sendai, Japan]. The author is also grateful to Mr. N. Hoshi and Y. Sato (DENJIKEN) for assisting in the experiments.
The author declares that there are no competing interests.
Authors’ original submitted files for images
Below are the links to the authors’ original submitted files for images.
About this article
Cite this article
Abe, S. Formation of Nb2O5 matrix and Vis-NIR absorption in Nb-Ge-O thin film. Nanoscale Res Lett 7, 341 (2012) doi:10.1186/1556-276X-7-341
- Phase Mixture
- Composite Thin Film
- Optical Absorption Edge