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- Table of Contents
Journal of Sensors
Volume 2009 (2009), Article ID 790476, 9 pages
Schottky Junction Methane Sensors Using Electrochemically Grown Nanocrystalline-Nanoporous ZnO Thin Films
1Department of Electronics & Telecommunication Engineering, IC. Design & Fabrication Centre, Jadavpur University, Kolkata 700032, India
2Department of Physics, Chemistry and Biology, Linkoping University, SE-581 83 Linköping, Sweden
Received 29 December 2008; Accepted 1 July 2009
Academic Editor: Giorgio Sberveglieri
Copyright © 2009 P. K. Basu et al. 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.
Nanocrystalline-nanoporous ZnO thin films were prepared by an electrochemical anodization method, and the films were tested as methane sensors. It was found that Pd-Ag catalytic contacts showed better sensing performance compared to other noble metal contacts like Pt and Rh. The methane sensing temperature could be reduced to as low as by sensitizing nanocrystalline ZnO thin films with Pd, deposited by chemical method. The sensing mechanism has been discussed briefly.
It is well known that gas sensing performance of sensors can be improved by incorporating noble catalyst metal into the nanocrystalline metal oxide-based matrix. A number of reports [1–3] have been published on nanocrystalline ZnO thin films to improve the methane sensing performance. The development of a low-temperature methane detector using nanocrystalline ZnO-based chemical gas sensors with noble metal catalytic contacts is an important proposition. The challenge is to attain lower detection limit, short response time, and long-term stability of the gas sensors. Nanocrystalline ZnO thin films demonstrate remarkable gas-sensing properties when the crystallite size becomes comparable to Debye length. Nanocrystalline and porous materials with controlled composition are of increasing interest in methane sensing because of their large surface to volume ratio that enhances the adsorption kinetics and the reaction between methane and adsorbed oxygen.
Recently it was [1–6] reported that methane-sensing temperature varies between 100°C and 250°C depending upon whether the ZnO thin film is grown electrochemically or by sol-gel method and upon the nature of the catalytic metals. But these relatively high temperatures for detection of methane are still not suitable for applications in the coalmines. In this work, nanocrystalline ZnO thin films were prepared by electrochemical anodization of high-purity Zn (99.99%). While using Pt catalytic metal electrode methane sensing could be achieved at 240°C Pd-Ag (26%), and Rh electrodes could bring down the temperature to 210°C. But the temperature could be brought down to 100°C by incorporating Pd modification of the nanocrystalline ZnO thin film and by using Pd-Ag catalytic metal Schottky contact. In this communication, a comparative study between ZnO Schottky devices with different catalytic metal contacts and the effect of adding Pd to the nanoporous ZnO are presented.
The noble metal/ZnO Schottky structure using nanocrystalline ZnO thin film, prepared by electrochemical anodization of Zn, was studied for gas sensing. A properly cleaned high-purity Zn foil of thickness 0.5 mm was taken as anode and platinum foil as cathode with 18 mm separation between the two electrodes and 0.3 M oxalic acid as electrolyte. A calomel electrode was taken as the reference. A 10 V potentiostatic power supply (Princeton Applied Research, Scanning Potentiostat-362, USA) was used during anodization. Sensitization of the grown ZnO films was performed by dipping into 0.01 M weak acidic aqueous solution of PdCl2 for 2 seconds followed by baking at 110°C for 10 minutes and annealing at 300°C in air for 30 minutes. Pt, Pd-Ag (26%) and Rh catalytic metals of thickness 0.2 m were deposited on ZnO films by e-beam evaporation using Al metal mask for Schottky contacts. The Zn substrate beneath the ZnO film was used as ohmic contact. Electrical connections were performed by using fine copper wire and silver paste. The schematic of the Schottky sensor structure is shown in Figure 1. In order to study the gas sensing properties high-purity methane, nitrogen, and synthetic air were used. For accurate control of the gas flow rate throughout the experiments, mass flow controller and mass flow meters (Digiflow, USA) were used. The current-voltage characteristics of the sensors were studied by a Keithley model 6487 Pico ammeters-voltage source.
3. Results and Discussions
The XRD and the FESEM (Field Effect Scanning Electron Microscopy) picture of the anodized ZnO thin films are shown in Figure 2. The average crystal size, the pore diameter, and the thickness are summarized in Table 1.
The V-I characteristics of the Schottky sensors were recorded at all the temperatures of measurements, and the magnitude of the response () was calculated from these data. The response () is defined as the ratio of the change of current in presence of methane in N2 or air to the current in N2 or air at constant voltage, both in the forward bias mode and expressed as
where is the current in presence of gas and is the current in N2 or air.
Figure 3(a) shows response versus temperature curves of the Schottky sensors with the unsensitized ZnO films using 1% CH4 in pure N2. For Pt contact the maximum response was obtained at 240°C while for Pd-Ag and Rh contacts the maximum response was obtained at 210°C. For all three types of contacts the maximum response was obtained at 0.4 V bias, as shown in Figure 3(b). This may be significant for low power consumption of the sensor devices. Figure 4 shows the response versus temperature curves with 1% CH4 in pure N2 and in synthetic air, respectively. It is observed that the response of the sensors is higher in nitrogen compared to that in synthetic air.
In case of the Schottky gas sensors, catalytic noble metals were taken as electrode contacts. At an elevated temperature, oxygen molecules are weakly bonded to the catalytic metal (Pt, Pd-Ag, and Rh) and are dissociated to oxygen atoms that are weakly adsorbed on the metal surface. The metal-oxygen complex subsequently dissociates The oxygen atoms then undergo a spillover process and finally form negatively charged surface ions by gaining electrons from the surface of ZnO, thereby yielding a high electrostatic potential in the junction [7–9]. The space charge region, being depleted of electrons, is more resistive than the bulk. The methane response mechanism with a noble metal/metal oxide Schottky junction is not so well understood and spectroscopic studies are needed in order to reveal the reaction pathways that may be different for different temperatures and even vary with the gas concentration. Here we present three possible mechanisms of gas sensors. The first is dissociative adsorption of CH4 to produce H and CHx (X = 3) on the noble metal surface and reaction with adsorbed atomic oxygen to produce water. Furthermore, the H or CHx spills over to the metal oxide and reacts with chemisorbed ionic oxygen to produce water and free electrons that increase the current through the junction. If the device is operated at a temperature of 100°C, which is normally the case for methane sensing, the water formed desorbs rapidly from the surface [10–12] (see reactions (3)):
A second possibility is that due to high solubility and rapid diffusivity of hydrogen through catalytic metal, it reaches the catalytic metal/metal oxide interfaces and produces an interfacial dipole layer. The electrically polarized potential at the interface also lowers the work function of the noble metal and thus reduces the barrier height. Such sensing mechanism is summarized in Figure 5, where the reduction of the barrier height upon exposure to the reducing gas is shown. The adsorbed hydrogen atoms may, as a third possibility, passivate the interface states at the noble metal/metal oxide interface, preventing them from pinning the Fermi level. The passivated interface thus might cause a decrease in the barrier height. Due to this lowering of barrier height, the current through the junction increases [6, 13], yielding thereby a high response.
Palladium (Pd), Silver (Ag), Platinum (Pt), and Rhodium (Rh) are the most common metal catalysts that are used to improve the gas-sensing properties. Here Pt, Pd-Ag, and Rh catalysts were used for gas sensing applications. A Pd-Ag (26%) alloy metal contact was used instead of pure Pd. The reason is that the phase transition from α phase of pure palladium to phase hydride occurs at low H2 concentration at 300 K and it is an irreversible process . This will damage the sensor due to peeling-off of Pd. Moreover, the response time of more than 10 minutes for pure Pd contact sensors, as reported in the literature , is too long to allow real-time monitoring of flowing gas streams. To overcome these problems Pd was alloyed with 26% Ag for CH4 sensing. Pd-Ag thin film is attractive for use  because of the low rate of hydride formation, not much hindrance against hydrogen diffusivity, greater solubility of hydrogen, higher energy barrier due to OH formation and superior mechanical properties as compared to pure Pd. The alloy has quite high rate of hydrogen adsorption in the temperature range 30°C–100°C that is important for fast responding gas sensors.
It can be observed that Rh gives higher response than Pd-Ag and Pt (Rh Pd-Ag Pt) because the catalytic effect of dissociation of methane is higher than Pd and Pt . Also the OH formation rate influences the size of the response as discussed below. In literature, it can also be found that the catalytic activity of Pd and Pt for methane dissociation is more or less the same . But Figures 3 and 4 show a higher response of Pd-Ag alloy than Pt that implies that the catalytic activity of Pd-Ag is higher than that of pure Pd. In case of synthetic air that is shown in Figure 4 it can be noticed that the response is somewhat reduced. Since oxygen is already chemisorbed to a large extent on the noble metal surface the adsorption sites for methane is likely to be reduced. So dissociated hydrogen reacts with chemisorbed oxygen to produce H2O molecules instead of diffusing into the noble metal/ZnO junction, thereby yielding a weaker response. Since oxygen adsorption is most favorable on Pt it gives the most reduced performance in presence of synthetic air as compared to the other two metals, as shown in Figure 4. Similarly the OH formation energy of Rh is higher than Pd-Ag and Pt [18–21]. Thus this is another reason why the Rh catalytic metal contact gives higher response than Pd-Ag and Pt. The transient response of the sensors recorded in presence of different methane concentrations (0.01%, 0.05%, 0.1%, 0.5%, and 1%) and at 0.4 V bias is shown in Figure 6. From the transient response cycles the response and recovery time were calculated and are summarized in Table 2. The response time is defined here as the time to reach 67% of the saturation value of the current. After the gas pulse is cut off the time required to reduce the current to 67% is defined as the recovery time. It can be observed from Table 2 that the Pd-Ag contact shows shorter response time than Pt and Rh contacts, which may be due to the higher solubility and diffusivity of H in Pd-Ag compared to Rh and Pt and therefore H takes shorter time to reach the Pd-Ag/ZnO junction compared to that for Pt/ZnO and Rh/ZnO junctions, but it may also be because of more favorable chemistry on the Pd-Ag surface. This is because the catalytic metal/ZnO is most likely highly porous due to a rather thin catalytic metal (200 nm) and a highly porous ZnO, which makes diffusion through the metal a noncritical parameter. It should also be noted in Table 2 that the recovery times for Pd-Ag and Pt are about the same. This is most likely because of the back reaction between hydrogen and oxygen for water formation, as well as carbon dioxide formation, on the catalytic metal surface both in the case of nitrogen and synthetic air. It is almost impossible to attain oxygen leakage free systems for measurements at atmospheric pressure in the laboratory. It can be inferred that Pd-Ag alloy is the most suitable catalytic metal amongst the three for methane sensing using the Pd-Ag/ZnO Schottky junction.
There are very few reports on metal oxide based methane gas sensors with high response and fast response and recovery . The reported sensor structures [1–5] on oxide based semiconductors operating in the resistive mode and at high temperatures showed longer response and recovery time. This is not suitable for low temperature applications, particularly in the mining environment. It may also incur higher power consumption and short battery lifetime.
To improve the sensing performance, the surface of ZnO thin films was chemically modified with Pd. From FESEM the surface morphology and the pore size were revealed for both unmodified and modified ZnO surfaces (Figure 7). It was observed that there is little or no difference in the surface morphology after treatment with PdCl2 solution . The presence of Pd was confirmed by XPS studies. Table 3 shows the improvement of methane sensing parameters after Pd surface modification of ZnO thin film.
The variations of the response with operating temperature and with biasing voltage using 1% methane in nitrogen and in synthetic air are shown in Figure 8. It is observed from the figure that maximum response was obtained at 100°C and at 3 V. It is further observed that the response is higher in pure nitrogen than in synthetic air.
For the nanocrystalline structure the adsorption energy [22, 23] is considerably lower, and the presence of dispersed Pd nanoparticles over ZnO surface further reduces it. As a result the sensors respond at considerably lower temperature. It is worth mentioning here that imperfect structural orientation of the polycrystalline sensing layer (ZnO) also modulates the gas adsorption behavior and thus the sensing parameters .
Figure 9 represents the transient response for different concentrations of methane at 100°C using nitrogen and synthetic air as carrier gases. The response time and recovery time with increasing methane concentrations as derived from the transient response curves are shown in Table 4.
It is apparent from the table that response time is shorter than recovery time that is true also for the cases in Tables 2 and 3. The Pd-Ag/ZnO surface seems to be favorable for the adsorption kinetics at the catalytic metal and Pd-Ag/ZnO interface, compare Tables 3 and 4, the same way the recovery time is longer than the response time for all cases in Tables 2–4. It is interesting to note that the recovery time in Table 4 is about the same in nitrogen and oxygen, which supports the earlier discussion that the back reaction is the same in nitrogen and oxygen atmosphere due to oxygen leakage into the system.
It should be noted that the sensing of methane at 100°C for Pd-Ag/ZnO might be suitable for practical applications due to the high response, speed of response, and recovery, because there is no accumulation of water molecules on the sensor surface at 100°C .
We tested the long-term stability of the Schottky sensor for 33 days in presence of 1% methane in nitrogen at 100°C, and the results are shown in Figure 10(a). It is evident from the figure that the sensors show more or less stable performance with a negligible variation of current over the above-mentioned period in a nitrogen atmosphere. We also tested the stability in synthetic air; see Figure 10(b) for 8 hours and a fairly good stability was obtained. The long-term stability in air needs to be further tested since this is the realistic atmosphere for a methane leak detector.
Our investigation confirms that methane can be detected at as low a temperature as 100°C using Pd-Ag alloy as the Schottky contact to nanocrystalline ZnO thin film, obtained by anodization of Zn and surface modified by using noble metal, for example, Pd. Nanocrystalline ZnO thin films, after Pd surface modification, showed improved sensing characteristics like large response, short response and recovery time. The stability of the sensor structure obtained in this study indicates that the sensor might be good for methane sensing in the coalmine environment.
One of the authors (P. K. Basu) gratefully acknowledges CSIR, Government of India, for a Senior Research Fellowship (SRF).
- P. K. Basu, P. Bhattacharyya, N. Saha, H. Saha, and S. Basu, “The superior performance of the electrochemically grown ZnO thin films as methane sensor,” Sensors and Actuators B, vol. 133, no. 2, pp. 357–363, 2008.
- P. Bhattacharyya, P. K. Basu, H. Saha, and S. Basu, “Fast response methane sensor using nanocrystalline zinc oxide thin films derived by sol-gel method,” Sensors and Actuators B, vol. 124, no. 1, pp. 62–67, 2007.
- P. K. Basu, P. Bhattacharyya, N. Saha, H. Saha, and S. Basu, “Methane sensing properties of platinum catalysed nano porous zinc oxide thin films derived by electrochemical anodization,” Sensor Letters, vol. 6, no. 1, pp. 219–225, 2008.
- P. Bhattacharyya, P. K. Basu, C. Lang, H. Saha, and S. Basu, “Noble metal catalytic contacts to sol-gel nanocrystalline zinc oxide thin films for sensing methane,” Sensors and Actuators B, vol. 129, no. 2, pp. 551–557, 2008.
- P. Bhattacharyya, P. K. Basu, H. Saha, and S. Basu, “Fast response methane sensor based on Pd(Ag)/ZnO/Zn MIM structure,” Sensor Letters, vol. 4, no. 4, pp. 371–376, 2006.
- P. K. Basu, S. K. Jana, H. Saha, and S. Basu, “Low temperature methane sensing by electrochemically grown and surface modified ZnO thin films,” Sensors and Actuators B, vol. 135, no. 1, pp. 81–88, 2008.
- S. W. Hla, P. Lacovig, G. Comelli, A. Baraldi, M. Kiskinova, and R. Rosei, “Orientational anisotropy in oxygen dissociation on Rh(110),” Physical Review B, vol. 60, no. 11, pp. 7800–7803, 1999.
- A. Rothschild and Y. Komem, “The effect of grain size on the sensitivity of nanocrystalline metal-oxide gas sensors,” Journal of Applied Physics, vol. 95, no. 11, pp. 6374–6380, 2004.
- S. L. Tait, Z. Dohnalek, C. T. Campbell, and B. D. Kay, “Methane adsorption and dissociation and oxygen adsorption and reaction with CO on Pd nanoparticles on MgO(1 0 0) and on Pd(1 1 1),” Surface Science, vol. 591, no. 1–3, pp. 90–107, 2005.
- M.-S. Liao, C.-T. Au, and C.-F. Ng, “Methane dissociation on Ni, Pd, Pt and Cu metal (111) surfaces—a theoretical comparative study,” Chemical Physics Letters, vol. 272, no. 5-6, pp. 445–452, 1997.
- V. R. Shinde, T. P. Gujar, and C. D. Lokhande, “Enhanced response of porous ZnO nanobeads towards LPG: effect of Pd sensitization,” Sensors and Actuators B, vol. 123, no. 2, pp. 701–706, 2007.
- M. Lofdahl, C. Utaiwasin, A. Carlsson, I. Lundstrom, and M. Eriksson, “Gas response dependence on gate metal morphology of field-effect devices,” Sensors and Actuators B, vol. 80, no. 3, pp. 183–192, 2001.
- C. Xu, J. Tamaki, N. Miura, and N. Yamazoe, “Relationship between gas sensitivity and microstructure of porous ,” Journal of the Electrochemical Society, vol. 58, p. 1143, 1990.
- R. C. Hughes, W. K. Schubert, T. E. Zipperian, J. L. Rodriguez, and T. A. Plut, “Thin-film palladium and silver alloys and layers for metal-insulator-semiconductor sensors,” Journal of Applied Physics, vol. 62, no. 3, pp. 1074–1083, 1987.
- M. Wang and Y. Feng, “Palladium-silver thin film for hydrogen sensing,” Sensors and Actuators B, vol. 123, no. 1, pp. 101–106, 2007.
- S. Eriksson, M. Nilsson, M. Boutonnet, and S. Järås, “Partial oxidation of methane over rhodium catalysts for power generation applications,” Catalysis Today, vol. 100, no. 3-4, pp. 447–451, 2005.
- V. A. Drozdov, P. G. Tsyrulnikov, V. V. Popovskii, N. N. Bulgakov, E. M. Moroz, and T. G. Galeev, “Comparative study of the activity of Al-Pd and Al-Pt catalysts in deep oxidation of hydrocarbons,” Reaction Kinetics and Catalysis Letters, vol. 27, no. 2, pp. 425–427, 1985.
- R. Löber and D. Hennig, “Interaction of hydrogen with transition metal fcc(111) surfaces,” Physical Review B, vol. 55, no. 7, pp. 4761–4765, 1997.
- E. P. J. Mallens, J. H. B. J. Hoebink, and G. B. Marin, “The reaction mechanism of the partial oxidation of methane to synthesis gas: a transient kinetic study over rhodium and a comparison with platinum,” Journal of Catalysis, vol. 167, no. 1, pp. 43–56, 1997.
- L. Opara, B. Klein, and H. Zuchnerh, “Hydrogen-diffusion in ,” Journal of Alloys and Compounds, vol. 253-254, pp. 378–380, 1997.
- I. Lundström, H. Sundgren, F. Winquist, M. Eriksson, C. Krantz-Rülcker, and A. Lloyd-Spetz, “Twenty-five years of field effect gas sensor research in Linköping,” Sensors and Actuators B, vol. 121, no. 1, pp. 247–262, 2007.
- S. Liu, K. Takahashi, K. Fuchigami, and K. Uematsu, “Hydrogen production by oxidative methanol reforming on Pd/ZnO: catalyst deactivation,” Applied Catalysis A, vol. 299, no. 1-2, pp. 58–65, 2006.
- H. Zhang, R. L. Penn, R. J. Hamers, and J. F. Banfield, “Enhanced adsorption of molecules on surfaces of nanocrystalline particles,” Journal of Physical Chemistry B, vol. 103, no. 22, pp. 4656–4662, 1999.
- V. Khranovskyy, J. Eriksson, A. Lloyd-Spetz, and R. Yakimova, “Oxygen absorption effect on the sensitivity and material stability of ZnO nanostructured films,” in Proceedings of IEEE Sensors, pp. 874–877, Lecce, Italy, October 2008.