Metal oxides have often been utilized for commercial gassensor materials.[1] In spite of their high sensitivity, their high power consumption due to high resistance has been a serious drawback. Conducting polymers have also been tried, since they operate at room temperature and have good sensitivity and reproducibility. However, the effects of humidity and degradation by ultraviolet irradiation, in particular, have hindered further practical applications. [2] Recently, carbon nanotube (CNT)-based gas sensors have received a great deal of attention. Nanosized CNT-based gas sensors of the field-effect-transistor type have superb sensitivity at room temperature due to a drastic change in the electrical conductivity upon the adsorption of various gases. [3,4] Despite such advantages, however, their application is still limited by a long recovery time and a complex fabrication process. In particular, the single-walled carbon nanotubes (SWNTs) used for gas sensors must be semiconducting.[5] However, the presence of both metallic and semiconducting carbon nanotubes in conventional powder samples reduces the reproducibility and/or yield of the devices. The issue here is to introduce an easy fabrication process of gas sensors whilst still retaining high sensitivity. To meet this criterion, we fabricated a gas sensor from a nanocomposite by polymerizing pyrrole monomer with SWNTs. Polypyrrole (Ppy) was prepared by a simple and straightforward in situ chemical polymerization of pyrrole mixed with SWNTs, and the sensor electrodes were formed by spin-casting SWNT/Ppy onto pre-patterned electrodes. Ppy was uniformly coated on the wall of the SWNTs to increase the specific surface area. The measured resistivity was greatly reduced due to the presence of the conductive SWNT network, whereas the specific surface area was increased about threefold. The sensitivity of the gas sensor fabricated with the SWNT/Ppy nanocomposite towards NO 2 gas, as measured by a direct voltage divider at room temperature, was very high and similar to that of the fabricated SWNTs alone.[3] Figure 1 shows the typical field-emission scanning electron microscope (FESEM) images of the Ppy, SWNTs, and SWNT/ Ppy nanocomposite formed by a simple in situ chemical polymerization. Pure Ppy synthesized without SWNTs (Fig. 1a) shows a typical granular morphology. The granule size of the pure Ppy is about 0.2±0.3 lm. The purified SWNTs shown in Figure 1b are entangled and crosslinked with a typical bundle diameter of 20 nm. The pyrrole monomer becomes anchored to the carbon nanotube walls during polymerization, covering them completely, as shown in Figure 1c. The inset of this figure shows the shape of the electrodes formed on the substrate. The two electrodes are separated by 500 lm. The specific surface areas of Ppy, SWNTs, and SWNT/Ppy nanocomposite were 23, 100, 65 m 2 g ±1 , respectively. [6] The surface area of the COMMUNICATIONS
This study characterizes the effects of incident infrared (IR) radiation on the electrical conductivity of graphene oxide (GO) and examines its potential for mid-IR detection. Analysis of the mildly reduced GO (m-GO) transport mechanism near room temperature reveals variable range hopping (VRH) for the conduction of electrons. This VRH behavior causes the m-GO resistance to exhibit a strong temperature dependence, with a large negative temperature coefficient of resistance of approximately -2 to -4% K(-1). In addition to this hopping transport, the presence of various oxygen-related functional groups within GO enhances the absorption of IR radiation significantly. These two GO material properties are synergically coupled and provoke a remarkable photothermal effect within this material; specifically, a large resistance drop is exhibited by m-GO in response to the increase in temperature caused by the IR absorption. The m-GO bolometer effect identified in this study is different from that exhibited in vanadium oxides, which require added gold-black films that function as IR absorbers owing to their limited IR absorption capability.
The sensing characteristics of conducting polymers to several volatile organic compounds were investigated with a UV-Vis-NIR spectrophotometer, dynamic contact angles measurement and scanning probe microscopy (SPM). When gases were absorbed, the polypyrrole (PPy) and polyaniline (PANi) exhibited positive and negative sensitivity, respectively. The PPy-based sensor demonstrated decreasing conductivity while the PANi sensor exhibited increasing conductivity when the polarity of the molecules absorbed increased. PPy film has an hydrophilic property while the PANi film a hydrophobic one. These changes in polymer conductivity, it is speculated, are due to the interruption of free carrier movement or the generation of polarons by the absorbed molecules.
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