Effects of functionalization of TiO2 nanotube array sensors with Pd nanoparticles on their selectivity.

This study compared the responses of Pd-functionalized and pristine titanate (TiO2) nanotube arrays to ethanol with those to acetone to determine the effects of functionalization of TiO2 nanotubes with Pd nanoparticles on the sensitivity and selectivity. The responses of pristine and Pd-functionalized TiO2 nanotube arrays to ethanol gas at 200 °C were ~2877% and ~21,253%, respectively. On the other hand, the responses of pristine and Pd-functionalized TiO2 nanotube arrays to acetone gas at 250 °C were ~1636% and 8746% respectively. In the case of ethanol sensing, the response and recovery times of Pd-functionalized TiO2 nanotubes (10.2 and 7.1 s) were obviously shorter than those of pristine TiO2 nanotubes (14.3 and 8.8 s), respectively. In contrast, in the case of acetone sensing the response and recovery times of Pd-functionalized TiO2 nanotubes (42.5 and 19.7 s) were almost the same as those of pristine TiO2 nanotubes (47.2 and 17.9 s). TiO2 nanotube arrays showed the strongest response to ethanol and Pd functionalization was the most effective in improving the response of TiO2 nanotubes to ethanol among six different types of gases: ethanol, acetone, CO, H2, NH3 and NO2. The origin of the superior sensing properties of Pd-functionalized TiO2 nanotubes toward ethanol to acetone is also discussed.

Introduction

Titanate (TiO2) is one of the most widely studied semiconductor materials. Formation of TiO2 nanotubes was reported for the first time by Hoyer [1]. Anodic formation of titania nanotubes was demonstrated for the first time by Zwilling et al. [2,3]. Over the past two decades, a range of applications including dye-sensitized solar cells, batteries, photocatalysts and chemical sensors have been explored [4-7]. TiO2 nanotube (NT) arrays have been used to detect O2, NO2, H2, CO, ammonia, formaldehyde, acetone, ethanol, chloroform, humidity and other gases [6,8-20]. TiO2 NT gas sensors showed high sensitivity and a rapid response at relatively low temperatures [7,20].

The functionalization of semiconductor gas sensors with metal catalysts is one of the most commonly used techniques for enhancing the sensitivity of gas sensors. The electrical response of a gas sensor to the target gas depends strongly on the efficiency of catalytic reactions of the surface of gas sensor material with the target gas. The sensitivity of gas sensors can be enhanced considerably by modifying the catalytic activity of the gas sensor material using metal catalysts such as Pd, Pt, Au and Ag. Table 1 lists some references for metal catalyst-functionalized TiO2 nanotube sensors in the literature [21-27]. Four kinds of metal catalyst-functionalized TiO2 nanotube arrays were assessed to detect a range of gases, but their sensing properties toward ethanol gas were not reported. The mechanism through which the sensitivity of a gas sensor is enhanced by functionalizing the sensor material with metal catalysts is well established [28-31]. Basically, a combination of electronic and chemical mechanisms is used to explain the enhanced sensitivity. Nevertheless, the effects of metal catalysts on the selectivity of sensors are not completely understood.

Table 1.

Summary of the metal catalyst-functionalized TiO2 nanotube gas sensors in the literature.

Type of Nanostructures	Functionalization Material	Gas	Reference
TiO2 nanotube arrays	Pt	SO2SOF2, SO2F2	[21]
Anodic TiO2 nanotube films	Pt, Pd	H2	[22]
TiO2 nanotubes	Ni, Pd	CO2, methane	[23]
TiO2 nanofilms	Pd	H2	[24]
TiO2 nanotube arrays	Au	CO	[25]
TiO2 nanotubes arrays	Au	NO2	[26]
TiO2 nanotubes	Au	toluene	[27]

In this study, the sensing properties of pristine and Pd-functionalized TiO2 nanotube array sensors toward ethanol and acetone were compared to determine the effects of the metal catalyst on the sensitivity and selectivity of the sensors. The differences in the sensitivity and sensing speed of pristine and Pd-functionalized TiO2 nanotube arrays between the two gases were analyzed based on the sensing mechanism of metal catalyst-functionalized oxide semiconductor nanostructures. Pd has been most commonly adopted as a metal catalyst because of its excellent catalytic behavior.

Results and Discussion

Figure 1a and the inset in Figure 1a show the top view and cross-sectional view scanning electron microscopy (SEM) images, respectively, of a Pd-functionalized TiO2 nanotube array synthesized by anodization followed by annealing at 500 °C for 2 h. The length and diameter of the titanium nanotube were 300–400 nm and 70–120 nm, respectively. Figure 2 shows X-ray diffraction (XRD) patterns of the sample (annealed at 500 °C) obtained at an anodizing voltage of 50 V. This suggests that the phases present are anatase TiO2 (JCPDS Card 89-4921), titanium (Ti) (JCPDS Card 89-5009) and palladium (Pd) (JCPDS Card 89-4897). The as-synthesized TiO2 nanotube array sample was amorphous, but crystallized after annealing at 500 °C and coating with Pd. According to the literature, TiO2 crystallizes above 300 °C [32,33]. The clear sharp peaks observed in the XRD patterns indicate the presence of a crystalline phase. According to the literature, with increasing calcination temperature, TiO2 crystallizes into two phases: rutile and anatase with anatase dominant at lower temperatures. After annealing at 500 °C for 2 h, TiO2 nanotubes were crystallized completely, but stable rutile and metastable anatase TiO2 phases coexisted. In addition to the peaks from TiO2 four peaks characteristic of metal Ti and two small reflection peaks characteristic of metal Pd were identified, which were indexed as the (002), (101), (102) and (201) reflections from tetragonal-structured Ti and the (200) and (220) reflections from face-centered cubic-structured Pd. The presence of Pd nanoparticles on the TiO2 nanotube surface was confirmed further by transmission electron microscopy (TEM). High-resolution TEM (HRTEM) image (Figure 1d) revealed a spherical Pd particle with a diameter of ∼7 ± 4 nm on the surface of TiO2 nanotube. A close examination revealed two different fringe patterns: one with a spacing of 0.195 nm corresponding to the interplanar spacing of the Pd (200) lattice plane and the other with a spacing of 0.35 nm corresponding to the interplanar spacing of the TiO2 (101) lattice plane. The corresponding selected area electron diffraction (SAED) pattern (Figure 1e) showed a concentric ring pattern, suggesting that both TiO2 nanotubes and Pd nanoparticles were polycrystalline, even if they showed local fringe patterns. The concentration of Pd in the Pd-functionalized TiO2 nanotube array was estimated to approximately 1% based on the low-magnification TEM and HRTEM images.

Figure 1.

(a) Scanning electron microscopy image of Pd-functionalized TiO2 nanotubes; (b) Low-magnification transmission electron microscopy (TEM) image of a typical Pd-functionalized TiO2 nanotube; (c) High-resolution TEM image and (d) Corresponding selected area electron diffraction pattern of a typical Pd-functionalized TiO2 nanotube; (e) X-ray diffraction pattern of Pd-functionalized TiO2 nanotubes.

Figure 2.

Electrical responses of the gas sensors fabricated from (a) pristine TiO2 nanotubes and (b) Pd-functionalized TiO2 nanotubes to 10–3000 ppm C2H5OH gas at 200 °C; (c) Enlarged part of the pristine TiO2 nanotube curve in Figure 2a at 100 ppm C2H5OH; (d) Enlarged part of the Pd-functionalized nanotube curve in Figure 2b at 100 ppm C2H5OH at 200 °C; (e) Electrical response of pristine TiO2 nanotubes to 100 ppm CH3COCH3 at 250 °C; (f) Electrical response of Pd-functionalized TiO2 nanotubes to 100 ppm CH3COCH3 at 250 °C. Note: The sensing test temperature for C2H5OH differs from that for CH3COCH3.

Figure 2a,b shows the dynamic electric responses of pristine and Pd-functionalized TiO2 nanotube arrays, respectively, to a reducing gas ethanol pulses at concentrations of 10, 50, 100, 200, 500, 1000, 1500, 2000, 2500 and 3000 ppm at 200 °C. The current increases reversibly upon each ethanol pulse. The electrical behavior of the sensors was consistent, recovering their original currents without hysteresis after repeated exposure to different ethanol gas concentrations.

The pristine TiO2 nanotube arrays showed responses of approximately 235, 468, 691, 986, 1334, 1657, 2009, 2355, 2693 and 2877% to 10, 50, 100, 200, 500, 1000, 1500, 2000, 2500 and 3000 ppm ethanol, respectively. In contrast, the Pd-functionalized TiO2 nanotube arrays showed responses of approximately 297, 796, 1590, 3132, 4997, 7196, 9984, 14,079, 17,072 and 21,253% to 10, 50, 100, 200, 500, 1000, 1500, 2000, 2500 and 3000 ppm ethanol, respectively. Pd-functionalization increased the response to 3000 ppm ethanol gas by more than seven fold.

Figure 2c,d shows the enlarged parts of the dynamic response curves of pristine and Pd-functionalized TiO2 nanotube arrays in Figure 2a,b, respectively, to 100 ppm ethanol at 200 °C drawn to illustrate the moments of gas input and gas stop. Similarly, Figure 2e,f presents the response curves of pristine and Pd-functionalized TiO2 nanotube arrays, respectively, at 100 ppm acetone at 250 °C. The sensing data at 200 °C and 250 °C for ethanol and acetone, respectively, are shown in these figures because the best sensing data was obtained at those temperatures. The responses of pristine and Pd-functionalized TiO2 nanotube arrays to ethanol gas at 200 °C were ∼986% and ∼3132%, respectively (Supporting Information, Table S1). On the other hand, the responses of pristine and Pd-functionalized TiO2 nanotube arrays to acetone gas at 250 °C were ∼473% and 1152%, respectively. In the case of ethanol sensing, the response time and recovery time of Pd-functionalized TiO2 nanotubes (10.2 and 7.1 s) were shorter than those of pristine TiO2 nanotubes (14.3 and 8.8 s), respectively. In contrast, the sum of the response time and recovery time of Pd-functionalized TiO2 nanotubes (65.1 s) to acetone was similar to that of pristine TiO2 nanotubes (62.2 s). A comparison of Figure 2c with Figure 2e showed that both the response and recovery times of pristine TiO2 nanotubes toward ethanol gas were significantly shorter than toward acetone gas. On the other hand, a comparison of Figure 2d with Figure 2f showed that both the response time and recovery time of Pd-functionalized TiO2 nanotubes toward ethanol gas were also far shorter than toward acetone gas. The following conclusion can be extracted from the above sensing data: Functionalization of TiO2 nanotubes with Pd enhances both the sensitivity and sensing speed significantly toward ethanol gas, whereas it enhances only the sensitivity toward acetone gas.

Figure 3a shows the responses calculated from Figure 2a as a function of ethanol concentration. A linear relationship was observed between the response and ethanol concentration in the ethanol gas concentration range below 3000 ppm. The response of a semiconductor is commonly expressed as R = A [C] + B, where A and B, n (usually equal to 1), and [C] are constants, exponent, and the target gas concentration, respectively [34]. Data fitting resulted in the following equations for responses to ethanol: R = 0.83 [C] + 634.34 and R = 6.61 [C] + 859.4 for pristine and Pd-functionalized TiO2 nanotubes, respectively. Data fitting also gave the equations for the responses to acetone: R = 0.49 [C] + 300.86 and R = 2.44 [C] + 248.20 for pristine and Pd-functionalized TiO2 nanotubes, respectively. A comparison of the response curves showed that both the pristine and Pd-functionalized TiO2 nanotubes had higher sensitivity to ethanol than to acetone. The Pd-functionalized TiO2 nanotubes showed a superior response and a greater increasing rate of the response to ethanol or acetone gas concentration to pristine TiO2 nanotubes. The difference in the response of the pristine TiO2 nanotubes between ethanol and acetone is not so big, but the difference in response of the Pd-functionalized TiO2 nanotubes between ethanol and acetone was much larger.

Figure 3.

(a) Responses of pristine and Pd-functionalized TiO2 nanotubes to ethanol or acetone gas as a function of the ethanol or acetone concentration; (b) Responses of pristine and Pd-functionalized TiO2 nanotubes to ethanol or acetone gas as a function of temperature.

Figure 3b shows the responses of the pristine and Pd-functionalized TiO2 nanotubes to ethanol and acetone as a function of temperature. The pristine and Pd-functionalized TiO2 nanotubes showed the strongest responses to ethanol and Pd-functionalized TiO2 nanotubes showed a higher response ratio compared to pristine TiO2 nanotubes at 200 °C. In addition, Pd-functionalized TiO2 nanotubes showed the strongest responses to ethanol at 250 °C. Attempts were made to measure the responses to ethanol and acetone at higher temperatures, but they failed because of the excessive noise in the dynamic response curve at the temperatures.

Over the past two decades TiO2 nanotube arrays were mostly studied to detect hydrogen [18,35,36]. They were commonly operated at temperatures as high as several hundred degrees Celsius, because of their unsatisfactory sensing performances at low temperatures. However, the high operating temperatures are not desirable for many applications, particularly those involving flammable environments or requiring low power operation. Titania nanotube arrays were also used to fabricate humidity sensors [19] and low-temperature oxygen sensors operating at 50–300 °C [20]. On the other hand, studies on the sensing properties of TiO2 nanotube arrays to other gases such as ethanol, acetone, CO, NH3 and NO2 have been relatively fewer compared to H2, O2 and humidity. We compared the responses of pristine and Pd-functionalized TiO2 nanotubes to ethanol with those to other gases as shown in Figure 4 to see the selectivity of TiO2 nanotubes in gas sensing. The responses of the pristine and Pd-functionalized TiO2 nanotubes to ethanol were far higher than those to other gases, respectively. The responses of the pristine and Pd-functionalized TiO2 nanotubes to acetone were far lower than those to ethanol, even if they were higher than the responses to other gases such as H2, CO, NH3 and NO2. At present, it is not well understood why pristine and Pd-functionalized TiO2 nanotubes showed stronger responses to ethanol than to hydrogen. We surmise that it is due to relatively low sensing test temperature (200 °C). If the sensing test had been done at a far higher temperature, it would have given different results. In particular, the ratio of the response of Pd-functionalized TiO2 nanotubes to that of pristine TiO2 nanotubes is the highest for ethanol (∼8.8), the next highest for acetone (∼2.8) and less than 2.0 for other four gases (Supporting Information, Table S2), suggesting that Pd functionalization is most effective in improving the response of TiO2 nanotubes to ethanol among the six different kinds of gases.

Figure 4.

Comparison of responses of pristine and Pd-functionalized TiO2 nanotubes to different gases.

Upon exposure to air the oxygen species (O2−, O− and O2−) are adsorbed by the TiO2 surface, which creates a depletion layer in the surface region of TiO2 nanotubes by extracting electrons from the conduction band of TiO2 as follows [37]:

Upon exposure to ethanol (C2H5OH) gas a large amount of electrons are produced through the following reactions [38], returning to TiO2 and then transferring to Pd.

These reactions reduce the electron depletion layer width in the TiO2 surface region.

A combination of electronic and chemical mechanisms is commonly used to explain the metal catalyst-induced enhancement of sensitivity [39-41]. In the electronic mechanism, the enhanced sensitivity was based on the modulation of the width of the depletion layer formed around each Pd particle or the conduction channel due to changes in the oxidation state of the Pd accompanying oxygen adsorption and desorption [29]. Pd nanoparticles act as electron acceptors on TiO2 nanotube surfaces, resulting in a further decrease in depletion layer width. Consequently, the change in current is larger in Pd-functionalized TiO2 nanotubes than in pristine TiO2 nanotubes, leading to enhanced response. On the other hand, in the chemical mechanism, the enhanced sensitivity is based on the excellent catalytic dissociation ability of Pd. Pd activates the catalytic dissociation of oxygen and ethanol (or acetone) molecules because it is a far superior dissociation catalyst to TiO2. Of these two mechanisms the further enhancement in the response to ethanol by Pd-functionalization than to acetone could be explained by the electronic mechanism as follows:

The amount of electrons (6e−) produced by the oxidation reaction of 1 mol of ethanol according to Equation (2) is larger than that (4e−) produced by the oxidation reaction of the same amount (1 mol) of acetone (CH3COCH3) according to Equation (5) [42]:

Therefore, a narrower depletion layer is created upon exposure to ethanol than to acetone, assuming that the amounts and concentrations of the two target gases are the same.

Experimental Section

Anodization was performed to synthesize TiO2 nanotube arrays using a conventional two-electrode cell system. The as-treated Ti plates were used as the working electrode and a platinum sheet (2 × 1.5 cm2) with a platinum wire was used as the counter-electrode. The anodization potential (anodization voltage = 60 V, current = 1–3 mA) was applied using a potentiostat interfaced with a computer. The electrolyte (dimethyl sulfoxide (DMSO) + 2 vol % HF (48%)) was stirred with a magnetic flea during the anodization process. Details of the synthesis procedure of TiO2 nanotube arrays are reported elsewhere [43]. Subsequently, the synthesized TiO2 nanotube array were immersed in ethanol/(10 mM) PdCl2 solution and irradiated with UV laser (λ = 254 nm, I = 1.2 mW/cm2) for 30 min. To induce crystallization of TiO2 nanotube arrays and allow the Pd thin films on the nanotube surfaces to agglomerate into Pd nanoparticles, the products (Pd-capped TiO2 nanotubes) were annealed at 500 °C in an O2 atmosphere (flow rate = 30 sccm) for 2 h. The collected nanotube array samples were examined by scanning electron microscopy (SEM, Hitachi S-4200, Tokyo, Japan), transmission electron microscopy (TEM, Philips CM-200, Eindhoven, The Netherland) and X-ray diffraction (XRD, Philips X'pert MRD diffractometer, Eindhoven, The Netherland). The crystallographic structure was determined by glancing angle XRD with Cu-Kα radiation (0.15406 nm) at a scan rate of 4°/min, and a 0.5° glancing angle with a rotating detector.

For the sensing measurement, gold wires were connected directly to both the electrodes and a TiO2 nanotube array synthesized on a Ti thin foil substrate using Ag paste. The gas sensing properties of a single TiO2 nanotube sensor measured using a home-built computer-controlled characterization system consisting of a test chamber, a sensor holder, a Keithley 2602 source meter, mass flow controllers and a data acquisition system. The test gas was mixed with dry air to achieve the desired concentration and the flow rate was maintained at 200 sccm using mass flow controllers. The current flowing through the samples was measured at 200 or 250 °C using a Keithley 2602 source meter under 50% relative humidity (RH). A given amount of C2H5OH (>99.99%) gas was injected into the testing tube through a microsyringe to obtain a C2H5OH concentration of 10–3000 ppm, and the electrical current in the nanotubes was monitored. The response of the TiO2 nanotube sensors is defined as (Ig − Ia)/Ia, where Ia and Ig are the electrical currents in the sensors in air and target gas, respectively. Details of the arrangement of the electrodes in the TiO2 nanotube gas sensor and the sensing test procedure are reported elsewhere [43]. The response time is defined as the time required for the variation in electrical resistance to reach 90% of the equilibrium value after injecting the gas and the recovery time is defined as the time needed for the sensor to return to 90% above the original resistance in air after removing the gas.

Conclusions

The responses of pristine (∼2877%) and Pd-functionalized (∼21,253%) TiO2 nanotube arrays to ethanol gas at 200 °C were higher than those of pristine (∼1636%) and Pd-functionalized (∼8746%) TiO2 nanotube arrays, respectively, to acetone gas at 250 °C. In the case of ethanol sensing, the sensing speed of Pd-functionalized TiO2 nanotubes were shorter than that of pristine TiO2 nanotubes, whereas in the case of acetone sensing, the sensing speed of Pd-functionalized TiO2 nanotubes was the same as that of pristine TiO2 nanotubes. TiO2 nanotube arrays showed the strongest response to ethanol and Pd functionalization was the most effective in improving the response of TiO2 nanotubes to ethanol among six different types of gases: ethanol, acetone, CO, H2, NH3 and NO2. Of the electronic and chemical mechanisms, the further enhancement in response to ethanol rather than acetone by Pd-functionalization can be explained only by electronic mechanism. The amount of electrons (6e−) produced by the oxidation reaction of 1 mol of ethanol is larger than that (4e−) produced by the oxidation reaction of the same amount (1 mol) of acetone (CH3COCH3), resulting in superior sensing properties toward ethanol to acetone.