Eu-doped ZnO (ZnO:Eu3+) thin films deposited by RF magnetron sputtering have been investigated to establish the effect of annealing on the red photoluminescence. PL spectra analysis reveal a correlation between the characteristics of the red photoluminescence and the annealing temperature, suggesting efficient energy transfer from the ZnO host to the Eu3+ ions as enhanced by the intrinsic defects levels. Five peaks corresponding to 5D0–7FJ transitions were observed and attributed to Eu3+ occupancy in the lattice sites of ZnO thin films. As a proof of concept a dye sensitized solar cell with ZnO:Eu3+ thin films of high optical transparency was fabricated and tested yielding a PCE of 1.33% compared to 1.19% obtained from dye sensitized solar cells (DSSC) with pristine ZnO without Eu produced indicating 11.1% efficiency enhancement which could be attributed to spectral conversion by the ZnO:Eu3+.
Zinc oxide has emerged as a crucial member of the group II–VI family owing to its attractive properties such as a wide band gap (3.37 eV) and a large excitonic binding energy (60 meV)1,2,3,4 as well as being environmental friendly material5. Highly transparent and conductive ZnO thin film with nanostructured morphologies is an extensively researched field for potential technological applications, especially for the use in various electronic and optoelectronic devices, such as surface acoustic wave devices, gas sensing applications, transparent coating and solar cell applications6. Various growth techniques have been reported including chemical vapor deposition (CVD), thermal oxidation, pulsed laser deposition, spray pyrolysis and sputtering7. Among these methods, magnetron sputtering of transparent conductive oxides remains a promising technique capable of low temperatures deposition of thin films with good optical and electronic properties with a special advantage of the scalability to large areas8.
The use of high quality II–VI semiconductor nanocrystals as dopant hosts for optically active impurities acting as luminescence centers has gained a lot of interest due to efficient luminescence even at room temperature9,10. Such dopants are rare-earth ions which are optically and magnetically active in the semiconductor (ZnO) host crystals11 such that, strong interactions between the quantum-confined carriers and localized electrons on impurities from impurity-doped ZnO will produce efficient photoluminescence. This is because direct excitation of the parity forbidden 4f–4 f transitions of Eu3+ is generally inefficient compared with the host absorption in UV region12. Among the rare earth ions, Eu has emerged as an attractive dopant for red emission in the range of 620–740 nm and the resulting related luminescence lines have been reported to be strongly dependent on the structural quality and thermal cycling of the host material13. Upon resonance excitation hot carriers-impact excitation, or carriers injected in the p-n junction structure, ZnO semiconductor has the potential to display luminescence over wavelengths from UV to infrared with potential applications in electroluminescence (EL) and cathodoluminescence (CL) displays14.
In the present work, we report on the structural, morphological and optical changes on the preparation of transparent conducting thin of ZnO:Eu3+ thin film. Thus, establish the dependence of the enhancement of 5D0 → 7F2 transition in PL spectrum on annealing temperature. In this study, Eu doped ZnO thin films are grown using RF magnetron sputtering at room temperature. The films were subsequently studied after annealing in argon in the range 500–900 °C. Moreover, the blue and green emissions in ZnO:Eu3+ nanostructures related to native ZnO defect are also discussed.
Thin film growth
ZnO (97%): Eu (3%) (99.99% purity) target of diameter 76 mm and thickness 6 mm sourced from Semiconductor Wafer, Inc. (SWI) have been used for thin film deposition. This was carried out using R.F. magnetron sputtering system. The substrate used were p-type (001) Si, quartz (for optical measurements) and FTO coated glass (for device fabrication). The substrates were thoroughly cleaned with organic solvents and dried before loading in the sputtering system. The vacuum chamber was evacuated using a rotary roughing pump to a base pressure of 2 × 10−2 mbar before further pump down by turbomolecular pump to 1.8 × 10−5 mbar. Magnetron sputtering was carried out in an argon gas atmosphere supplied into the chamber through a constant precision leak valve at a flow rate of 13.0 sccm.
The surface morphology of the films were characterized using FEI Nova Nanolab 600 SEM. Rutherford backscattering spectrometry (RBS) measurements were performed to determine the thickness and distribution profiles of Eu3+ ions in the ZnO matrix annealed 500 °C using 4He+ particles of energy 1.6 MeV at a backscattering angle of 165° (IBM geometry). The crystallographic properties of the ZnO films was carried out using GXRD Bruker D8 Discover, 40 kV, 40 mA using a 8.0 keV Cu-Kα radiation. The scanning range of 2θ was varied from 10° to 80° at a low scanning rate of 1.2°/minute. Photoluminescence measurements were carried out using a Horiba LabRAM HR spectrometer with a 150 lines/mm grating and an excitation wavelength of 244 nm from a frequency doubled Lexel argon ion laser
Solar cell fabrication
As a proof of concept of transparent conducting and spectral conversion layer, a dye sensitized solar cell was fabricated using FTO electrode annealed at 500 °C chosen to avoid glass softening at higher temperatures. For sensitization, the ZnO and ZnO:Eu3+ films were quickly thoroughly deeply dipped into a dye solution (3.0 × 10−4 M mixture of the ruthenizer 535-bisTBA (N-719) in methanol) before drying for 12 h at room temperature. The counter electrode was composed of a thin layer of Pt (50 nm) sputter coated on a clean FTO substrate.
The electrode with ZnO and ZnO:Eu3+ thin film photoanode was placed face up on a flat surface, and the counter electrode placed on top of it. The two opposing glass plates were then offset from one another to enable complete coverage of photoanode by the counter electrode. The redox electrolyte solution (I−/I3−), made of 0.6 M methylhexylimidazolium iodide, 0.1 M iodine, 0.5 M tert-butylpyridine, and 0.1 M lithium iodide in 3-methoxypropionitrile, was then placed on the edges of the plates before the liquid was drawn into the space between the electrodes via capillary action. An epoxy adhesive was utilized to hold/seal the electrodes together. The entire thin film making and characterization is summarized in Scheme 1.
Results and discussion
Figure 1 shows the SEM image of ZnO:Eu3+ annealed at different temperatures ranging between 500–900 °C.
The micrographs of both pristine and annealed thin films shown in Fig. 1 indicate a uniform deposition of compact columnar growth of ZnO:Eu3+ thin films. The films have fine grain structure with average grain size, calculated from Scherrer’s formula, in the range of 51.5 to 70.4 nm. The increase in temperature leads to an enhancement in the grain size and coverage. This is coupled with an increase in surface roughness as witnessed using tapping mode AFM (see Supplementary Fig. S1). This change may be attributed to the stress in the thin films prompting a disturbance of the columnar growth.
Rutherford Backscattering Spectroscopy Measurements
The elemental and percentage composition and distribution of the Eu3+ ions in the ZnO thin film was established using Rutherford Backscattering Spectroscopy as shown in Fig. 2 for film annealed at 500 °C. The elements could also be confirmed by EDS (see Supplementary Fig. S2).
Figure 2 shows the raw (black curve) and simulated (red curve) RBS spectra of ZnO:Eu3+ thin film annealed at 500 °C. The vertical arrows indicate the scattering energies of the elemental constituents in the film. The simulation of the experimental spectra has been carried using the XRump code15 and the results of their depth profile are presented in Table 1.
The simulation of the XRump code yields a film thickness of 357 nm (graded) and it is in agreement with values obtained from the surface profilometer (356.6 nm). The presence of Si at depths within the ZnO:Eu3+ film is attributed to diffusion (Thermal Diffusivity 0.9 cm2/sec) and atomic intermixing at the interface. The total average Eu composition is ∼1% with majority being found at a depth of 278 nm (upto layer 4).
X-Ray Diffraction Analysis
The room temperature XRD pattern of ZnO:Eu3+ thin film annealed at various temperatures are depicted in Fig. 3. It is evident that the ZnO:Eu3+ film has a predominantly hexagonal wurtzite structure (JCPDS database No: 00–003–0888). For different annealing temperatures, the detected diffraction angles (2θ), FWHM of the (100) peak, d values, grain sizes, dislocation densities and tensile strains in the films are tabulated in Table 2.
Additionally, it is observed that there are no diffraction peaks associated with europium oxides or other impurities in the XRD pattern of Fig. 3. This is an indication that the Eu3+ ions are probably incorporated into the ZnO lattice. All peaks in the XRD pattern are of ZnO and could be readily indexed as the hexagonal wurtzite ZnO phase with lattice constants (a) 3.24890 Å and (c) 5.20620 Å, which are in good agreement with the reported data in the literature16,17,18. Usually the diffraction peaks of Eu3+ doped ZnO samples may have a lower angle (2θ) compared to undoped ZnO thin film, in our case a shift of about 0.5 (2θ) as a result of the larger ionic radius of Eu3+ (0.95 Å) in comparison to that of Zn2+ (0.74 Å)19 is observed.
Upon annealing of ZnO:Eu3+ thin films, the prominent (100) peak is gradually shifted to higher 2θ (31.74° to 32.04°) while its FWHM gradually decreases from 2.82 to 1.45 nm for (500–700 °C) temperature range, an indication of enhanced crystallinity with annealing.
The residual strain decreased from 9.03 × 10−3 to 6.08 × 10−3 with increasing temperature up to 700 °C. Above 900 °C the strain increases to 7.68 × 10−3. Without annealing, surface atoms have less energy hence low surface mobility, resulting in generation of defects in ZnO films. On annealing at 500–700 °C, the atoms gain sufficient mobility to engender atomic rearrangement during crystallization of ZnO. The effect is further supported by reduction in the FWHM. Further increase in annealing temperature to 900 °C resulted in breaking of partially coordinated Zn-O bonds on the surface rather than enabling the atoms to move freely to their corresponding stable sites, producing defects and stress in ZnO film hence the increase in strain and dislocation density20.
Figure 4 represents the transmittance spectra in (%) of the as deposited and annealed ZnO:Eu3+ thin films on quartz substrates capable of withstanding the high annealing temperatures without softening. This was done as a function of wavelength. The rapid cutting in intensity near 372 nm is attributed to the band edge absorption. The increase in transmittance at λ < 330 nm can be attributed to structural changes in glass at high temperature (900 °C).
From Fig. 4, high transparency in the visible wavelength range was observed in all the thin films with a sharp ultraviolet absorption edge in the UV region approximately at 372 nm. This abrupt absorption edge coupled with excellent optical transmission within the visible range of the spectrum is an indication of the films of high quality. The interferential behavior of spectra is attributed to light reflectance occurring between ZnO:Eu3+ - substrate interface and ZnO:Eu3+ - air surface21. High transmittance of about 95% recorded is crucial to effective application into solar cells where highly transparent and conductive is major requirement of the electrodes in device application. It can be seen that as the annealing temperature increases, the absorption edge shift to lower energy. After doping with Eu3+ ions, a systematic low-energy shift occurs in the band gap, indicating that the optical band gap is narrowed22. As shown in Fig. 5, the UV-Vis transmission spectrum was used to obtain the change in optical band gap with annealing temperature. Then, we use the direct allowable electron transition between the highest occupied state of the valence band and the lowest unoccupied state of the conduction band when a photon of energy, hν, falls on the film. The absorption coefficient, α, is related to the optical bandgap energy, Eg, by Tauc equation:
where α is the absorption coefficient, hv is the incident photon energy, C1 is a constant, Eg is the optical gap energy, and the exponent m is 1/2 for allowed transition enabling absorption based on the Fermi Golden rules.
When the films are annealed from 500–700 °C, the optical bandgap is observed to decrease from 3.29 to 3.19 eV before a larger decrease to 3.103 eV upon annealing at 900 °C as shown in Fig. 5. The decrease in Eg is a show of enhanced films quality as the structural defects are annihilated23 such as decrease of the O vacancies24. This is in agreement with the experimental results of XRD analysis. The tailoring of the bandgap of semiconductors could also be attributed to the introduction of new energy levels in the band gap near conduction edge such as shallow level donor impurities25.
The Changes in the nanoscale energy level of the thin film structure may seriously affect the light emitting performance. The relationship between the structure and emission behavior of ZnO:Eu3+ thin films and the annealing temperature was investigated using PL. Figure 7 shows the photoluminescence spectrum of Eu-doped ZnO thin film in the range of 350–800 nm, depicting several energy bands relating to the transitions from excited 5D0 level to the 7FJ (J = 0, 1, 2, 3, 4) levels of the Eu3+ 4f6 configuration26. It is mainly shown that the spectrum of the 5D0–7F2 transition is modified when the annealing temperature is increased, which indicates that there is a structural rearrangement around the Eu3+ centers. This is consistent with the proposed conversion shown in Fig. 6.
From Figs. 6–7, the UV emission attributed to near-band-edge (NBE) exciton recombination and a broad deep level emission is depicted as discussed in our previous publication3. Figure 7 shows the PL spectra of films annealed at between 500–700 °C while Fig. 8 includes films annealed at 900 °C.
It can be seen from Fig. 7 that at 372 nm and 536 nm, the intensity of near-band edge emission and deep-level defect emission suddenly decreased, and then began to increase after 700 °C, while the emission of the 5D0–7F2 transition at 613 nm increasing is a confirmation of energy transfer from ZnO to Eu3+ ions27,28,29.
It can be seen from Fig. 8 that when annealing at 900 °C, sharp peaks are observed at the wavelengths of 576 nm, 594 nm, 613 nm, 651 nm, and 703 nm, which correspond to the inherent 4 f → 4 f transition of Eu3 + in the ZnO host. Eu3+ ‘s intrinsic 4 f → 4 f transitions are assigned to 5D0 - 7F0, 5D0 - 7F1, 5D0 - 7F2, 5D0 - 7F3, and 5D0 - 7F4 respectively19,30,31. The strong peak at 613 nm indicates the occupancy of Eu3+ ions at the antisymmetric site of the host ZnO19. According to Judd-Ofelt theory, if Eu3+ ions occupy the center of symmetry of the ZnO lattice, magnetic dipole transitions are allowed. In this case, and in accordance with the Laporte selection rule in 4f6 transition, the electric dipole transitions is prohibited. However, electric dipole transitions are allowed only when Eu3+ ions occupy a position without an inversion center and their strength is significantly affected by the symmetry in the local environment32. If Eu3+ ions occupy an inverse symmetric site in the lattice, the magnetic transition 5D0 - 7F1 (about 594 nm) will be the main transition. Therefore, the dominance of 5D0 - 7F2 transitions in the spectrum indicates the possibility of electrical dipole transitions. The ratio of intensity (5D0- 7F2)/(5D0 - 7F1) can be used to establish a measure of deformation based on the antisymmetric nature of the Eu3+ ion local environment. It is known that the lower symmetry around Eu3+ ions will produce a larger intensity ratio, which is called asymmetry factor or asymmetry ratio33. Due to the 5D0-7F2 transition at 900 °C, the red peak at 613 nm has a very high intensity, which confirms that the Eu3+ emission is parity and only deforms in the lattice environment and has no inversion symmetry32. Since this is a forced electric dipole transition, this transition is very sensitive to the annealing temperature. It is known that Eu3+ ions may occupy two positions, namely the internal and surface lattice positions of ZnO materials29,34,35. In theory, Eu3+ ions are doped into the internal lattice sites of ZnO, or located at the Zn substitution sites with C3v symmetry. The transition of J = 0 and J = 1 will be divided into two crystals-field energy levels (J = 0 → J = 0, J = 0 → J = 1), but as can be seen from Fig. 6, there are five peaks at 5D0-7Fj, which indicates that Eu3+ ions have been incorporated into a lower symmetry site than C3v36.
Application of ZnO:Eu3+ into Dye sensitized solar cells
Figure 9 shows J-V characteristics of dye sensitized solar cell fabricated and tested in air ambient as a proof of concept. The sputtered films on cleaned FTO were used as an electrode. ZnO and Eu doped ZnO was deposited on it and the films were annealed at 500 °C as high temperature would lead to softening of glass supporting FTO. The aim of the heat treatment was to get improved adsorption between the film and dye molecules. The thickness and the active area of the film used were approximated to 357 nm and 0.25 cm2 respectively.
The DSSC was made of a salt electrolyte sandwiched between a dye-sensitized a counter electrode (CE) and photoanode (working electrode)37. The Photoanode is composed of a layer of wide-band gap semiconductor that is mesoporous attached to the conducting glass. Although we used ZnO:Eu3+ as mesoporous semiconductor, other oxides may also be used such as TiO238,39,40. A thin layer of charge transfer dye was then adsorbed on the surface of the mesoporous ZnO:Eu3+ semiconductor. This photoanode section was then attached to the redox electrolyte or hole conductor. Eventually the device was completed by connecting the sensitized photoanode with the counter electrode (cathode) as shown in Fig. 9 (inset).
The DSSC with ZnO:Eu3+ yielded a better performance with PCE of 1.33% (Jsc = 4.56 mA cm−2, Voc = 0.59 V and FF = 49.3%), compared to the DSSC with pristine ZnO that produced a PCE of 1.19% (Jsc = 4.14 mA cm−2, Voc = 0.57 V, FF = 50.6%) indicating 11.1% efficiency enhancement. The enhancement in efficiency is attributed to spectral conversion by the Eu doped ZnO. The device performance values obtained were relatively low. This low performance could be attributed to the exposure of the materials to air during fabrication and testing process. This exposure was deliberate as a proof of concept that the device fabrication and testing carried out in air is indeed feasible.
We successfully report deposition of polycrystalline ZnO:Eu3+ thin films of high orientation on (001) Si, quartz and FTO coated glass substrate using RF magnetron sputtering technique. A systematic analysis of the film crystallization dynamics is carried out at elevated temperature annealing in Argon filled furnace. The deposited thin films showed good transparency that became even better with annealing making them suitable for solar cell applications. Scanning electron microscope (SEM), grazing incidence X-ray diffraction (GXRD), and the Photoluminescence (PL) were used to characterize the effect of the post-deposition annealing treatment on the structural properties of the ZnO:Eu3+ thin films. The results shows that a small amount of Eu has been successfully incorporated in the ZnO host matrix. Structural studies reveal that films deposited by sputtering have a better structural quality that is even enhanced with annealing the films. The thin films indicated an increasing grain size and roughness of ZnO:Eu3+ with annealing temperature between 500–900 °C as well as a shifted diffraction peak position. Finally, we incorporated the thin films into a dye sensitized solar cell fabrication as a proof of concept. The fabricated devices with ZnO:Eu3+ thin films showed a remarkable performance with better transparency and efficiency enhancement that we highly attributed to spectral conversion when incorporated as a bi-functional layer.
Kashif, M. et al. Effect of different seed solutions on the morphology and electrooptical properties of ZnO nanorods. Journal of Nanomaterials, 106 (2012)
Cao, B., Li, Y., Duan, G. & Cai, W. Growth of ZnO nanoneedle arrays with strong ultraviolet emissions by an electrochemical deposition method. Crystal growth & design 6(5), 1091–1095 (2006).
Otieno, F. et al. Structural and spectroscopic analysis of ex-situ annealed RF sputtered aluminium doped zinc oxide thin films. Journal of applied physics 122(7), 075303 (2017).
Li, Z. et al. Fabrication and morphology dependent magnetic properties of cobalt nanoarrays via template-assisted electrodeposition. RSC Advances 2(8), 3447–3450 (2012).
Zhong, W.-W. et al. Effect of annealing on the structure and photoluminescence of Eu-Doped ZnO nanorod ordered array thin films. Journal of Nanomaterials, 1 (2012)
Nouri, A., Beniaiche, A., Soucase, B. M., Guessas, H. & Azizi, A. Photoluminescence study of Eu+3 doped ZnO nanocolumns prepared by electrodeposition method. Optik-International Journal for Light and Electron Optics 139, 104–110 (2017).
Huang, G., Cui, X., Cao, R. & Mei, Y. Structural evolvement of ZnO nanoporous films fabricated using prolonged electrodeposition under pulsed voltages. Physics Letters A 375(42), 3716–3719 (2011).
Ellmer, K. Magnetron sputtering of transparent conductive zinc oxide: relation between the sputtering parameters and the electronic properties. Journal of Physics D: Applied Physics 33(4), R17 (2000).
Zeng, H. et al. Blue Luminescence of ZnO nanoparticles based on non‐equilibrium processes: defect origins and emission controls. Advanced Functional Materials 20(4), 561–572 (2010).
Zeng, H. et al. “White graphenes”: boron nitride nanoribbons via boron nitride nanotube unwrapping. Nano letters 10(12), 5049–5055 (2010).
Taguchi, S., Ishizumi, A., Tayagaki, T. & Kanemitsu, Y. Mn–Mn couplings in Mn-doped CdS nanocrystals studied by magnetic circular dichroism spectroscopy. Applied Physics Letters 94(17), 173101 (2009).
Najafi, M., Haratizadeh, H. & Ghezellou, M. The effect of annealing, synthesis temperature and structure on photoluminescence properties of Eu-Doped ZnO Nanorods. Journal of Nanostructures 5(2), 129–135 (2015).
Shi, J. et al. Effect of growth temperature on Eu incorporation in GaN powders. Journal of Crystal Growth 310(2), 452–456 (2008).
Jadwisienczak, W., Lozykowski, H., Xu, A. & Patel, B. Visible emission from ZnO doped with rare-earth ions. Journal of electronic materials 31(7), 776–784 (2002).
Kótai, E. Computer methods for analysis and simulation of RBS and ERDA spectra. Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 85(1-4), 588–596 (1994).
Sharma, S., Vyas, S., Periasamy, C. & Chakrabarti, P. Structural and optical characterization of ZnO thin films for optoelectronic device applications by RF sputtering technique. Superlattices and Microstructures 75, 378–389 (2014).
Lim, S., Kwon, S. & Kim, H. ZnO thin films prepared by atomic layer deposition and rf sputtering as an active layer for thin film transistor. Thin Solid Films 516, 1523–1528 (2008).
Wang, X. et al. The properties of Al doped ZnO thin films deposited on various substrate materials by RF magnetron sputtering. Journal of Materials Science: Materials in Electronics 23, 1580–1586 (2012).
Pal, P. P. & Manam, J. Structural and photoluminescence studies of Eu3+ doped zinc oxide nanorods prepared by precipitation method. Journal of Rare Earths 31(1), 37–43 (2013).
Pandey, S. K. et al. Influence of annealing temperature on ZnO thin films grown by dual ion beam sputtering. Bulletin of Materials Science 37(5), 983–989 (2014).
Ievtushenko, A. et al. High quality ZnO films deposited by radio-frequency magnetron sputtering using layer by layer growth method. Thin Solid Films 518(16), 4529–4532 (2010).
Swapna, R., SrinivasaReddy, T., Venkateswarlu, K. & Kumar, M. S. Effect of Post-Annealing on the Properties of Eu Doped ZnO Nano Thin Films. Procedia Materials Science 10, 723–729 (2015).
Yang, S., Liu, Y., Zhang, Y. & Mo, D. Investigation of annealing-treatment on structural and optical properties of sol-gel-derived zinc oxide thin films. Bulletin of Materials Science 33(3), 209–214 (2010).
Wang, J. et al. Oxygen vacancy induced band-gap narrowing and enhanced visible light photocatalytic activity of ZnO. ACS Applied Materials & Interfaces 4(8), 4024–4030 (2012).
Kumar, V. et al. Tunable and white emission from ZnO: Tb3+ nanophosphors for solid state lighting applications. Chemical Engineering Journal 255, 541–552 (2014).
Armelao, L. et al. The Origin and Dynamics of Soft X‐Ray‐Excited Optical Luminescence of ZnO. ChemPhysChem 11(17), 3625–3631 (2010).
Wang, M. et al. Synthesis and photoluminescence of Eu-doped ZnO microrods prepared by hydrothermal method. Optical Materials 31(10), 1502–1505 (2009).
Zeng, X., Yuan, J., Wang, Z. & Zhang, L.-d Nanosheet‐Based Microspheres of Eu3+‐doped ZnO with Efficient Energy Transfer from ZnO to Eu3+ at Room Temperature. Advanced Materials 19(24), 4510–4514 (2007).
Liu, Y. et al. Optical spectroscopy of Eu3+ doped ZnO nanocrystals. The Journal of Physical Chemistry C 112(3), 686–694 (2008).
Park, Y.-K. et al. Time-resolved spectroscopic study of energy transfer in ZnO: EuCl3 phosphors. Journal of Luminescence 78(1), 87–90 (1998).
Fang, T.-H. et al. Photoluminescence characteristics of ZnO doped with Eu3+ powders. Journal of Physics and Chemistry of Solids 70(6), 1015–1018 (2009).
Natarajan, V. et al. Photoluminescence, thermally stimulated luminescence and electron paramagnetic resonance of europium-ion doped strontium pyrophosphate. Materials Research Bulletin 39(13), 2065–2075 (2004).
Dorenbos, P. et al. 4f–5d spectroscopy of Ce3+ in CaBPO5, LiCaPO4 and Li2CaSiO4. Journal of Physics: Condensed Matter 15(3), 511 (2003).
Lima, S., Sigoli, F., Davolos, M. R. & Jafelicci, M. Jr. Europium (III)-containing zinc oxide from Pechini method. Journal of Alloys and Compounds 344(1-2), 280–284 (2002).
Liu, Y., Luo, W., Li, R. & Chen, X. Spectroscopic evidence of the multiple-site structure of Eu3+ ions incorporated in ZnO nanocrystals. Optics letters, 32(5), 566–568 (2007).
Shahroosvand, H. & Ghorbani-asl, M. Solution-based synthetic strategies for Eu doped ZnO nanoparticle with enhanced red photoluminescence. Journal of Luminescence 144, 223–229 (2013).
Patel, J., Mighri, F., Ajji, A. & Chaudhuri, T. K. Solution processed approaches for bulk-heterojunction solar cells based on Pb and Cd chalcogenide nanocrystals. Nano Energy 5, 36–51 (2014).
Vogel, R., Hoyer, P. & Weller, H. Quantum-sized PbS, CdS, Ag2S, Sb2S3, and Bi2S3 particles as sensitizers for various nanoporous wide-bandgap semiconductors. The Journal of Physical Chemistry 98(12), 3183–3188 (1994).
Perera, V. áS. An efficient dye-sensitized photoelectrochemical solar cell made from oxides of tin and zinc. Chemical Communications 1, 15–16 (1999).
Sayama, K., Sugihara, H. & Arakawa, H. Photoelectrochemical properties of a porous Nb2O5 electrode sensitized by a ruthenium dye. Chemistry of Materials 10(12), 3825–3832 (1998).
Jun, H., Careem, M. & Arof, A. Quantum dot-sensitized solar cells—perspective and recent developments: a review of Cd chalcogenide quantum dots as sensitizers. Renewable and Sustainable Energy Reviews 22, 148–167 (2013).
The authors would like to thank the University of the Witwatersrand, Material Physics Research Institute, School of Chemistry, School of Physics; the XRD and MMU facilities at Wits and NRF (South Africa -Grant No. 85675). Special thanks to GCRF- START: Synchrotron Techniques for African Research and Technology for postdoctoral funding provided by UKRI (Grant No. ST/R002754/1).
The authors declare no competing interests.
Publisher’s note Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
About this article
Cite this article
Otieno, F., Airo, M., Erasmus, R.M. et al. Annealing effect on the structural and optical behavior of ZnO:Eu3+ thin film grown using RF magnetron sputtering technique and application to dye sensitized solar cells. Sci Rep 10, 8557 (2020). https://doi.org/10.1038/s41598-020-65231-6
This article is cited by
Journal of Materials Science (2021)