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ISRN Materials Science
Volume 2012 (2012), Article ID 894072, 5 pages
Enhanced Size-Dependent Piezoelectricity in Nanostructured Films
Department of Computer Science, University of Verona, Strada Le Grazie, 15, 37134 Verona, Italy
Received 25 January 2012; Accepted 16 February 2012
Academic Editors: Y. Masuda and R. Mota
Copyright © 2012 V. Dallacasa. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
We have developed a nanogenerator that is driven by mechanical forces to produce continuous direct-current output. The nanogenerator was fabricated with titanium dioxide nanoparticle arrays forming a Schottky barrier with a conducting electrode with a small gap. Under uniaxial mechanical compression, nanogenerators have shown repeatable and consistent electrical outputs with energy-conversion efficiency of order of magnitude at least comparable to similar nanogenerators based on piezoelectric materials. Flexoelectricity due to inhomogeneous strain induced in the nanostructured film has been identified as one possible mechanism of the high apparent piezoelectricity in the nanoparticles. The approach presents an adaptable, mobile, and cost-effective technology for harvesting mechanical energy from the environment. At the present stage it offers a potential solution for powering nanodevices.
Recently, an approach for converting mechanical energy into electrical energy has been suggested by using piezoelectric zinc oxide (ZnO) nanowire arrays [1, 2]. This technique has illustrated the feasibility of utilizing inorganic nanomaterials with semiconducting and piezoelectric properties for nanogenerators. The conversion of energy can be achieved by creating a Schottky junction between ZnO and a metallic corrugated zigzag electrode which realizes a rectifying contact. Results have been obtained with ultrasound waves with typical output powers pW/mm2 and sound waves with typical intensity 100 decibels which generate electricity in the order of 1–50 mV. It is believed that various novel applications including devices for the recharging of mobile phones, the operation of micro and nanodevices, and for the energy storage in batteries and capacitors become possible if prototype devices can be optimized to enhance their power input. It has been estimated that the performance can be improved by two-three orders of magnitude .
In this paper we report results of TiO2-based nanogenerators operated under static mechanical forces. The output power of such nanogenerators can be attributed to piezoelectricity in the TiO2 nanoparticles due to the flexoelectric effect which is expected at the nanoscale [3–6] for systems which are non-piezoelectric in bulk form.
2. Generator Design and Fabrication
The overall layout of the generator is shown in Figure 1. A sandwich structure is obtained with an array of aligned TiO2 nanostructures of films between two conducting ITO/glass electrodes. The ITO coating enhanced the conductivity of the electrodes and at the same time created a Schottky contact at the interface of TiO2 and the top electrode.
2.2. Fabrication Process
The device was fabricated by the deposition of a nanostructured TiO2 film on a ITO/glass substrate that forms an electrode. A colloidal paste was prepared by starting from nanostructured commercial powders (Degussa) . To optimize the separation of TiO2 clusters, mechanical machining in aqueous phase, in organic phase, or both and/or sonication of a concentrated emulsion of TiO2 was used. Such emulsion was then applied to the ITO/glass substrates (Optical Filters Ltd., England). The deposition was achieved by a dr. blade or spray deposition method. To optimize the homogeneity of the film structure and its conductivity, a sintering procedure was used by heating the devices overnight at a temperature . With this technique, films with typical thickness 10–20 μm are obtained.
Detailed optical microscope inspection indicate that the final TiO2 films present a uniform distribution with tightly sinterized grains.
AFM microscopy indicates that at the μm scale the films are constituted by a disordered array in the xy plane with cusps (Figure 2). At larger resolution they exhibit a nanometric structure with nanocrystals having comparable dimension ~30 nm within the xy plane and in the z-direction, if they were distributed compactly, a surface density 1012 cm−2 on the average would result.
A similar nanostructure is revealed for the ITO electrode, with slightly smaller density 1010 cm−2 and diameter and height 100 nm and 5 nm, respectively (Figure 3).
Each of the structures appears as aligned nanocrystals distributed irregularly in size and orientation strongly resembling the configuration shown in Figure 1.
The top electrode was an ITO/glass identical to the substrate and completed the sandwiched structure.
Typical dimensions of the devices are or order cm2.
The commercial ITO/glass substrates and top electrodes (Optical Filters Ltd., England) have typical surface resistance 20 Ω and a resistivity ρ = 20·10−4 Ωcm, such values being compatible with those reported in the literature .
When used as the substrate for deposition of the oxide, the ITO structure acts as a template to the arrangement of the oxide on it. Good adhesion is obtained for TiO2 films indicating a good crystal structure matching.
From the other hand, when ITO is used as the top electrode, its nanometric array structure is penetrated on contact by the smaller TiO2 array leading to an optimized contact and good mechanical interaction with the film.
3. The Operating Principle
The physical principle for creating charges on the nanoparticles is a coupling of piezoelectric and semiconducting properties . Under external stress by the top electrode, a strain field is created in the nanoparticles. This results in an electric field along the z-direction inside the nanoparticle and on its surface through the piezoelectric effect. Under compression/dilation, the electric potential distribution is approximately between V−(V+) and V+ (V−) towards the top electrode.
The potential is created by the relative displacement of the Ti cations with respect to the O2 anions in the crystal structure; these ionic charges cannot freely move and cannot recombine without releasing the strain. The potential difference is maintained as long as the deformation is in place and no foreign free charges (such as from the ITO contact) are injected.
The positive (negative) voltage created by the charges acts as an applied bias on the top electrode leading to polarization of the Schottky diode at the interface and passage of current through the barrier. The current is the result of driven flow of electrons between the electrode and the semiconductor TiO2. The flow of the free electrons through the nanoparticle will neutralize the ionic charges distributed in the volume and on the surface of the nanoparticles and thus reduce the magnitudes of the potentials V+ and V−.
4. Measuring System
When the top electrode has a configuration as shown in Figure 1, by scanning the electrode back and forth, we can reproduce the processes discussed above. Under uniaxial stress, the electrode will exert both vertical and lateral forces on the nanoparticles, and there will be generation of electricity. During the scan nanoparticles may either be bent on making contact with the electrode (A- and D-type in Figure 1) or contact the electrode without being bent (B-type) or remain isolated without any contact (C-type). The B nanoparticles constitute a parallel resistance of the device; the C nanoparticles are an infinite resistance not entering in the process.
The ITO electrode in contact with the TiO2 array was manipulated by a probe station. Pressure was applied on the sandwich through a calibrated force gauge (Lutron Electronics) of capacity 49 N. The voltage and resistance have been measured by an high-impedance voltmeter (Kitley).
A typical device configuration was studied by positioning the ITO electrode on the nanostructure, and applying uniaxial compression stress the spacing was controlled to obtain a reasonable contact by the monitoring of the resistance of the junction. The pressing head of the gauge was of cylindrical form of diameter . In order to distribute the force over the whole junction, a rigid layer is interposed between the head and the top electrode. The actual area of the junction which is compressed is estimated not larger than 1 cm2, slightly larger than the head dimension due to the lateral propagation of the applied force but smaller than the area of the whole device. Variations of pressure in time can be obtained by manipulating the head of the gauge manually or electronically to study the response of the devices both in static and dynamical conditions. In the following we report results under uniaxial static compression.
In Figure 4, we report the measured voltage at the junction as a function of the applied force for N. The voltage exhibits a linear dependence at lower force, an indication of charge accumulation at the interface at increased pressing levels. At larger forces it departs from such linear law and finally degrades to the mV range, which can indicate enhanced charge screening.
A decrease of the junction resistance is also observed, indicating an enhanced carrier mobility trough the junction. A clear correlation of the trends of voltage and resistance with the sign of the stress results. Furthermore, the voltage at the top electrode has always positive (negative) sign with increasing (decreasing) force, a typical evidence of a piezoelectric effect. Spontaneous voltages are measured at nominally zero stress, which can be ascribed to residual compressing stress internal to the nanograins of the device. An example of measured values of the resistance and its fitting curve is reported in Figure 5.
Large fluctuations (from sample to sample and in the same sample) appear in the voltage and the resistance, accompanied by time relaxation towards equilibrium as well as large hysteretic behaviour. Typically, times of order of several minutes can be required to achieve stabilized values. These fluctuations arise from the setup of the junctions and are determined by the pressing condition of the top electrode on the oxide film.
The principal results obtained with such devices and the geometrical and electric parameters are summarized in Table 1.
The lower contact on the ITO/glass substrate may be assumed to be ohmic, as indicated by the employed deposition method, which is a standard one in the literature .
The capacitance of the system is ignored in the circuit in order to simplify the discussion about DC measurement. The capacitance of the junctions turns out to be of order of magnitude F.
Centrosymmetric dielectrics are not expected to polarize under mechanical strain. A nonuniform strain or the presence of strain gradients can, however, locally break inversion symmetry and induce polarization even in centrosymmetric crystals. This phenomenon is termed flexoelectricity [3–6].
With reference to Figure 1, at moderate pressure nanoparticles are deformed and acquire positive and negative charges on the surface along the compression direction. The positive charges in contact with the top electrode turn out to produce an applied forward bias at the Schottky barrier so that current will flow at the junction. On traversing the junction from ITO, electrons will screen the piezo charges at the interface thereby decreasing the potential. The effect will be higher the higher the polarization, that is the current at the junction.
In order to examine the existence of the barrier, we have used reported values of the work function and electron affinity of ITO and TiO2 respectively. Reported data for the work function of ITO are in the range 4.17–5.54 eV with an average 4.6–4.7 eV [9, 10]. Reported data for the electron affinity of TiO2 in nanoporous films are in the range 3.9–4.3 eV [11–13]. We thus expect a barrier of the order 0.5–0.6 eV, which compares with the results of the voltages measured at the junction.
The order of magnitude of the piezoelectric constant can be obtained from the accumulated charge by modeling the junction as a condenser. The piezoelectric constant can be defined by the equation , where Q and F are the piezoelectric induced charge and the applied force respectively. The electric potential can be written as , where A is the area of the junction, L the film thickness, and Q the total piezoelectric charge so that
The quantity can be deduced from the slope of experimental curve in Figure 4 which amounts to . So, for typical values A~1 cm2, , we obtain .
We likewise can derive the value of from the experimental results on resistance. On modelling the junction by a diode equation, the resistance will be given by where (kT/e), m being an ideality factor of the diode and T the absolute temperature, is the thermal voltage and , with Io the characteristic current parameter value of the diode. Since voltage and force are connected through the linear relation (1), we can transform ∆V into ∆F in the exponent in (2), so that with Aεoεr/dL. By using typical values as in (1), we find that the value corresponds to the order of magnitude evidenced by the fitting in Figure 5 provided requiring an ideality factor . This value is consistently found in these devices.
A summary of results on piezoelectric parameters is reported in Table 2.
A nanogenerator using TiO2 nanoparticles was developed and tested. The output power response that occurred when the device was exposed to static uniaxial stress was measured and compared to that of a nanogenerator using a ZnO film. The nanogenerator with TiO2 nanoparticles demonstrated a significant improvement over a nanogenerator without nanoparticles which can be attributed to flexoelectricity at nanoscale.
The number of nanoparticles that was active for producing electricity was limited by the multiple contacts between the nanoparticles and the electrode; thus, the output current was rather small in the present design. The nanogenerator can power few nanodevices which operate at 10 nW [14–16] in our current study.
These technical difficulties could be overcome by an optimized design to improve nanogenerator efficiency by patterned growth of high-quality uniform nanoparticle arrays. A 102–103 factor enhancement of the efficiency can be estimated on the basis of the fraction of active nanoparticles.
We thank Prof. D. Tonelli, Prof. M. Berrettoni, and Dr. E. Scavetta of the Department of Physical and Inorganic Chemistry, University of Bologna, for collaboration and advice on the deposition of oxides.
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