Research Article | Open Access
Sung Joon Min, Jin Woong Kim, Joon Hyub Kim, Joon Hyock Choi, Chan Won Park, Nam Ki Min, "Effect of Varying the Semiconducting/Metallic Tube Ratio on the Performance of Mixed Single-Walled Carbon Nanotube Network Gas Sensors", Journal of Nanomaterials, vol. 2017, Article ID 8761064, 9 pages, 2017. https://doi.org/10.1155/2017/8761064
Effect of Varying the Semiconducting/Metallic Tube Ratio on the Performance of Mixed Single-Walled Carbon Nanotube Network Gas Sensors
The sensing properties of mixed networks consisting of semiconducting and metallic single-walled carbon nanotubes (SWCNTs) have been found to largely vary depending on the ratio of semiconducting to metallic tubes. Solution-deposited 99% semiconductor-enriched nanotube networks exhibited a sensitivity of 1.908%/ppm, whereas the unenriched 66% and 90% enriched samples exhibited a sensitivity of 0.027%/ppm and 0.113%/ppm, respectively. These results suggest that it is extremely important to minimize the metallic pathways to achieve high sensitivity. After an oxygen plasma treatment, the unenriched 66% sample exhibited a 526% increase in sensitivity (0.142%/ppm) compared to the untreated one, whereas the 90% device demonstrated a sensitivity of 1.521%/ppm, which corresponds to an improvement in the sensitivity of 13.5 times the pristine 90% sample. In addition, the plasma-treated sensors exhibited a much faster response time than the untreated one. The significant improvement in the performance of the highly enriched network sensors was explained by the large increase in the anchoring sites for ammonia molecules on the surface of the semiconducting single-walled CNTs and the faster charge transfer from absorbed molecules.
Chemical and biological sensors have emerged as dynamic approaches for detecting specific analytes for environmental protection, medical diagnostics, food and industrial safety, and security. Such devices and systems are becoming an increasingly indispensable part of our daily lives because the detection or identification of unknown gases and vapors is critically important for improving and protecting human health, safety, quality of life, and the environment . Nanotechnology is expected to lead to the development of inexpensive, simple sensors or devices that can rapidly detect, identify, and quantify biological and chemical species [2, 3]. Owing to the diverse nature of their potential applications, such nanosensors could significantly impact multiple sectors of the economy including healthcare, pharmaceutical, agricultural, food, environmental, and consumer products [2–5].
One of the most successful nanosensors is based on carbon nanotube (CNT) networks. Randomly oriented or aligned networks of single-walled CNTs (SWCNTs) are a promising material for future nanoscale functional devices such as chemical and biological sensors [4, 6–8]. SWCNT-network-based sensors have been categorized into three groups: modification of the Schottky barrier at the metal/CNT interface [9, 10]; charge transfer between a nanotube and an adsorbed analyte [11, 12]; and capacitive gating of the nanotube [13, 14]. Although it does not matter which sensing mechanism is actually responsible for the operation of a SWCNT sensor, it is extremely important to have a percolative network of semiconducting (s) SWCNTs to achieve high performance because only s-SWCNTs exhibit significant changes in their electrical properties (conductance) due to the presence of absorbed molecules [15, 16]. For mixtures of metallic (m) and semiconducting nanotubes, m-SWCNTs can deteriorate the sensor performance owing to two effects. Namely, metallic tubes are relatively insensitive to their chemical environment and their interactions with other species  and electrically short the s-SWCNTs and the device if they form a percolating pathway between two electrodes. Thus, the electrical performance of SWCNT-network-based sensors is strongly influenced by the semiconducting/metallic tube ratio () within the SWCNT films.
Another factor that affects the sensitivity of the CNT sensors is the oxygenated functional groups attached to the sidewall of the SWCNT tubes. These oxygen-containing groups are found to significantly increase the interaction of CNTs with gas molecules [4, 17–20]. The CNT surface can be modified by changing its chemical composition using chemical and plasma treatments [21–23]. Both treatments introduce oxygenated functional groups into the SWCNTs but produce different effects on the metallic and semiconducting SWCNT surfaces [21, 24].
The typical SWCNT-network system is a mixture containing approximately one-third m-SWCNTs and two-thirds s-SWCNTs. This inhomogeneity often results in fabrication complexity, low sensitivity, and poorly reproducible sensor performance. Recently, semiconductor-enriched nanotubes have become commercially available, which makes it easy for research groups to explore device applications based on enriched CNT networks . Several experimental and theoretical studies have demonstrated excellent field-effect transistors (FETs) with a high on-state conductance and high on/off ratios using semiconductor-enriched CNT networks [26–28], but there have been few reports to date on the effects of and plasma treatments on the performance of semiconductor-enriched SWCNT-network sensors.
In this study, we fabricate ammonia gas sensors based on SWCNTs with different semiconducting content (typical SWCNT and 90% enriched and 99% enriched SWCNTs) and demonstrate the large improvement in the sensitivity to NH3 gas as a function of . Finally, the influence of the O2 plasma treatment on the static and dynamic performance of the highly semiconductor-enriched SWCNT-network sensors is evaluated using ammonia gas as a target analyte.
2. Materials and Methods
2.1. Fabrication of Ammonia Gas Sensors
SWCNT-network sensors with 3 mm × 8 mm size (active area = 9 mm2) were fabricated on glass substrates. The SWCNT networks used as chemiresistors were deposited on a 4-inch glass wafer, and interdigitated palladium electrodes were then deposited on top of the SWCNT-network. The normal unenriched SWCNT material was purchased from HanWha Nanotech (Korea) and consisted of 60–70 vol% SWCNTs produced by the arc discharge method using a Ni–Y catalyst. In addition, 90% and 99% semiconductor-enriched SWCNTs were obtained from NanoIntegris (USA). The SWCNT networks were deposited by using a solution method [29, 30]. First, the glass wafer was oxygen-plasma-treated and functionalized with amine-containing molecules (poly-L-lysine). The semiconductor-enriched SWCNT solution was subsequently dispensed onto the self-assembled-monolayer-modified surface and dried for 2 h. Atomic force microscopy (AFM) was used to record the topography and to measure the SWCNT film thickness. The typical SWCNT thickness derived from AFM line profiles was approximately 30 nm. Submonolayer films instead of continuous networks were formed for the 90% and 99% SWCNTs, as shown in Figures 1(c) and 1(d). Figure S1 (in Supplementary Material available online at https://doi.org/10.1155/2017/8761064) is a larger version of the SEM images for SWCNT shown in Figure 1. Next, for the interdigitated electrode and contact pad, a 50 nm thick palladium film was evaporated onto the SWCNT networks by a thermal evaporation system and patterned by lift-off with optical lithography using a negative photoresist. Finally, the SWCNT films were patterned using oxygen plasma etching.
2.2. Oxygen Plasma Treatment for Surface Functionalization
After patterning, some SWCNT networks were radio-frequency (RF) plasma-treated with oxygen gas under much lower plasma power than those applied during etching. The typical parameters optimized through several experiments were an O2 flow rate of 10 sccm, a substrate temperature of 25°C, and an RF power of 10 W for 10 s.
The sensors are labeled as unenriched 66%, 90% enriched, and 99% enriched, corresponding to the normal SWCNTs and the 90% and 99% semiconductor-enriched SWCNT networks, respectively, and the plasma-treated sensor devices are labeled as p-66% and p-90% enriched, respectively. The plasma-treated 99% enriched device was not tested because the SWCNT-network was completely etched away, even under very low power O2 plasma.
The sensors were placed in the test fixture attached to a gas manifold that had the capability of mixing several gases using nitrogen as the carrier gas. A detailed description of the flow system and resistance measurement is presented elsewhere . An LCR meter (test signal: 20 kHz and 1 ) was used to measure the ammonia gas-sensing properties of different SWCNT networks as a function of the ammonia gas concentration levels in a chamber with electrical feed-through. The NH3 gas concentration was varied in the range from 3.6 ppm to 64.2 ppm. Values with error bars (see Figures 3, 4, 5, and 7) represent the average and standard deviations of triplicate measurements performed on independently fabricated electrodes.
3. Results and Discussion
3.1. Characteristics of SWCNT Networks with NH3 Gas
The assembled devices from all three SWCNT networks were first tested to confirm the formation of ohmic contacts and stability under ambient conditions and were then exposed to NH3 at different concentrations to demonstrate sensor performance.
Figure 2 shows the typical current ()–voltage () characteristics of three SWCNT-network sensors ( = 66%, 90%, and 99%) recorded at room temperature before exposure to NH3 gas. As expected, all SWCNT-network devices exhibited very linear and symmetric behavior regardless of the value of , indicating the good ohmic Pd–SWCNT contacts had been achieved. Javey et al.  demonstrated that it is possible to obtain CNTFETs with zero Schottky barrier (SB) height for holes by using Pd contacts on semiconducting CNTs to realize the greatest benefit of SWCNTs. SWCNT devices with reliable ohmic contacts exhibit characteristics that are more similar to highly resistive devices because the transport is not limited by the contacts. The measured resistances for the three devices are 1 kΩ, 0.5 kΩ, and 2.4 kΩ, which include the wiring and contact resistances, but the SWCNT-network resistance is the dominant part of the observed sample resistance because of the good ohmic contact. Despite the low ratio of 66% SWCNT, the initial resistance of the device was higher than that of the 90% device. As noted in several papers [33, 34], contact resistance is inversely proportional to the length of the CNTs. The reversal of the initial resistance of the 90% SWCNT device is due to differences in the length of 66% (~20 nm) and 90% CNT (approximately 400 nm) provided by each company.
(a) Unenriched 66% SWCNT
(b) 90% enriched SWCNT
(c) 99% enriched SWCNT
The curves recorded after exposing three devices to different NH3 concentrations are also highly linear and symmetrical for the NH3 concentrations (3 to 42 ppm), as illustrated in the insets in Figures 3(a)–3(c). The resistances of these devices were calculated at a bias of 1 V and plotted as a function of the concentrations in Figures 3(a)–3(c). The unenriched 66% and 90% enriched SWCNT sensors exhibited a typical nonlinear characteristic for CNT-based gas sensors [8, 10, 35, 36], whereas the 99% enriched device exhibited a linear increase in resistance with increasing NH3 gas concentration, as shown in Figure 3(c).
3.2. Comparison of the Sensitivity
Figure 4 shows the calibrated responsiveness [, where is the steady-state resistance of the sensor when exposed to various gas concentrations, and is the device resistance in the outgassed state] as a function of the NH3 concentration at room temperature for all investigated sensors in the ammonia-concentration range of 3–42 ppm. A general linear response is observed with increasing NH3 concentration with a significantly greater responsiveness for the 99% enriched network compared to unenriched 66% and 90% enriched films. This suggests that a large is the most important factor for achieving a high sensitivity in mixed SWCNT-network-based gas sensors (see the following section).
Figure 5 compares the sensitivity (in %/ppm NH3) calculated from calibration slopes in Figure 4. The unenriched 66% and 90% enriched samples exhibited a sensitivity of 0.033%/ppm and 0.099%/ppm, respectively. The most important result is that the 99% enriched device exhibited a sensitivity 17.7 times higher than the 90% enriched device.
The semiconducting or metallic properties of SWCNTs stem from the variation of their electronic structure, which is composed of arm-chair and zigzag structure. In previously reported papers, the authors claimed that the charge transfer of NH3 gas does not depend on the structure of the CNTs  as well as the fact that the interaction between NH3 gas molecules and nanotube does not have a significant effect on the electronic structures of SWCNTs . Therefore, the unexpected large difference in sensitivity between 90% and 99% enriched samples is a consequence of the many s-SWCNTs being shorted by m-SWCNTs. The electrical transport through the SWCNT networks with a low is usually dominated by the metallic pathways because of their low resistivity, as shown in the equivalent electric circuit in the inset of Figure 5. As a result, the s-SWCNTs are shorted by m-SWCNTs; therefore, a few m-SWCNTs in a network can drastically weaken the sensing effect, even for a high enrichment of 90% s-SWNTs. This suggests that it is extremely important to have a percolative network consisting of only s-SWCNTs without metallic shorts to achieve high sensitivity.
3.3. Comparison of the Dynamic Response
An overall comparison of the measured response and recovery characteristics of the SWCNT-network sensors is presented in Figures 6(a)–6(c) when they were cycled between NH3 and N2 atmospheres (N2 → 22.6 ppm NH3 → N2). All response curves are normalized by the resistance before exposure to the analyte. As the observations suggest, the sensors demonstrated a long absorption time and furthermore an incomplete recovery of initial resistance during desorption process. They recovered 54% to 98% of the response after the NH3 flow was halted.
Table 1 summarizes the measured adsorption (90% point of the final steady-state resistance) and desorption (10% point of the final steady-state resistance) times for the three devices. The response time was found to be almost the same for the three sensors. However, the response time for each device degraded with increasing NH3 concentration. This perhaps indicates slow charge transfer from the NH3 molecules to the SWCNTs due to the gradual transition from monolayer to multilayer adsorption as the concentration increases. In addition, the devices with low recovered more slowly compared to high sensors. This may be attributed to the difference in the ammonia molecule-CNT binding mechanisms or energy. Several works [39–41] have showed that NH3 molecules may be absorbed into SWCNTs via both physisorption and chemisorption. An s-SWCNT has more sites for chemisorption than an m-SWCNT. When switching from an NH3 atmosphere to a N2 atmosphere, the NH3 molecules very weakly physisorbed on the surface are easily released by the kinetic energy of the incoming N2 gas molecules, leading to a reversible change in the device resistance. The chemisorbed molecules, however, cannot be broken by the N2 gas flow alone, causing a larger buildup in chemisorbed NH3 on the m-SWCNT surface and thus an irreversible change in the resistance .
3.4. Effect of the Oxygen Plasma Treatment on the Networks
The surface chemical composition of the SWCNTs has a strong influence on the gas absorption process and therefore the sensing properties. In previous works [24, 43], an O2 plasma treatment was found to introduce a number of oxygen-containing defects into the surface of the CNT film, and these functional groups are known to significantly increase the sensitivity to gases. Although many workers have studied CNT gas sensors functionalized using a plasma process, no reported effects of a plasma treatment on the SWCNT networks with different were found in the literature. The unenriched 66% and 90% enriched SWCNT-network sensors were only tested because the 99% enriched SWCNT-network sensor was completely etched away, even under very low power O2 plasma.
Figure 7(a) is full-scale XPS spectra for 66% and 90% s-SWCNT before and after plasma treatment. Based on previously reported work , the C1s peak is generally shown at about 285 eV, and the typical O1s peak appears at approximately 533.4 eV. Before the plasma treatment, the O/C ratio for the 90% s-SWCNT sample (178.92%) is very larger compared to that of the 66% s-SWCNT sample (36.86%). High O/C ratio contributes to the resistance change of the SWCNT film by the charge transfer induced by adsorption of NH3 molecules because polar NH3 molecules form strong hydrogen bonds with the oxygen atoms on the oxidized tube. After plasma treatment, the O/C ratio increased for both the 66% and 90% s-SWCNT samples, and especially the variation for 66% sample was dramatically large. These changes contribute significantly to the sensitivity and response time of the device.
Figure 8 shows the measured dynamic responses of the unenriched 66% and 90% enriched SWCNT-network sensors, and the reproducible responses measured at the same NH3 gas concentration are presented in Figure S2. After plasma treatment, both p-66% and p-90% samples exhibited a significant improvement in the responsiveness and response time compared to the equivalent untreated sensors.
Figures 9(a) and 9(b) compare the normalized sensitivity (in %/ppm NH3) and response time before and after plasma treatment for the unenriched 66% and 90% enriched devices. It is observed from Figure 9(a) that the amount of s-SWCNT content and the plasma activation significantly affect the sensitivity of the SWCNT gas sensors. The p-66% samples exhibited an increase in sensitivity from 0.027 to 0.142%/ppm after the plasma treatment. Furthermore, the p-90% enriched devices exhibited a sensitivity of 1.521%/ppm, which is approximately equal to an improvement in sensitivity of 13.4 times the untreated 90% enriched samples (0.113%/ppm) and 10.7 times the p-66% samples (see Figure SI, in Section S3). In addition, the two plasma-treated devices exhibited a large reduction in the response time of 70–78%, as shown in Figure 9(b). The significantly enhanced performance with the oxygen plasma-treated devices is related to the nature of the SWCNT surface. The plasma-treated SWCNTs have more oxygen-containing functional groups, especially carboxyl groups, which act as sites for gas-molecule chemisorption [16, 19]. Such anchoring sites formed on the CNT surface are known to significantly increase the electronic interaction of CNTs with gas molecules. This affects the SWCNT-network in two ways: faster charge transfer from the NH3 molecules adsorbed on the defect sites to the SWCNT bulk, causing a faster response time, or hole-carrier depletion , causing an increase in resistance () and thus sensitivity. The enhancement of sensitivity is much more pronounced for the p-90% enriched devices, suggesting that the semiconducting SWCNT-network is very sensitive to oxygen-containing functional groups, as compared to the metallic SWCNTs. In addition, the plasma-treated devices with high showed more slow response time than that with low . Although some researchers argue that m-SWCNTs with chemisorption sites increase response time , our result for concurrent reaction of s- and m-SWCNT may be attributed to the reason why the electrical properties of m-SWCNTs are relatively insensitive to the interaction with NH3 .
In this work, we explored the influence of varying and an oxygen plasma treatment on the static and dynamic characteristics of NH3 gas sensors based on randomly oriented mixed SWCNT networks. We found that there is a close relationship between of the SWCNT networks and the sensitivity of gas sensors based on these networks. The most important result is that the 99% semiconductor-enriched devices exhibit a much higher sensitivity compared to the 90% enriched device, suggesting that a few m-SWCNTs in a network can drastically weaken the sensing effect, even for high enrichment, and a percolative network consisting of only s-SWCNTs without metallic shorts is required to achieve high performance. We also demonstrated the effect of an oxygen plasma treatment on the highly semiconductor-enriched SWCNT-network sensors. After an oxygen plasma treatment, the 90% enriched SWCNT-network exhibited a much higher sensitivity to NH3 gas than unenriched 66% and pristine 90% enriched samples, showing that the O2 plasma treatment has a stronger influence on the semiconductor-enriched SWCNT-network than the normal unenriched network, possibly indicating that more oxygenated defects are created in the s-SWCNT-network than in the m-SWCNT-network. These results provide valuable insights into the role of and the plasma treatment towards achieving a large improvement in the performance of SWCNT-network gas sensors.
Conflicts of Interest
The authors declare that there are no conflicts of interest regarding the publication of this paper.
This study was supported by 2016 Research Grant from Kangwon National University (no. 520160103) and by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education (NRF-2015R1A6A3A04060326).
Figure S1: SEM images of (A) 66%, (B) 90% and (C) 99% enriched SWCNT films. Figure S2: The reproducible responses of 66% and 90% enriched SWCNT sensors before and after the oxygen plasma treatment at an NH3 concentration of 22.6 ppm. Figure S3: Sensitivity of (A) untreated and (B) oxygen plasma-treated SWCNT gas sensors.
- P. K. Sekhar, E. L. Brosha, R. Mukundan, and F. H. Garzon, “Chemical sensors for environmental monitoring and homeland security,” The Electrochemical Society Interface, vol. 19, no. 4, pp. 35–40, 2010.
- R. D. van Zee and G. S. Pomrenke, “Nanotechnology enabled sensing: report of the national nanotechnology initiative workshop,” 2009, http://www.nano.gov/sites/default/files/NNI-Nanosensors-stdres.pdf.
- S. K. Vashist, D. Zheng, K. Al-Rubeaan, J. H. T. Luong, and F.-S. Sheu, “Advances in carbon nanotube based electrochemical sensors for bioanalytical applications,” Biotechnology Advances, vol. 29, no. 2, pp. 169–188, 2011.
- T. Zhang, S. Mubeen, N. V. Myung, and M. A. Deshusses, “Recent progress in carbon nanotube-based gas sensors,” Nanotechnology, vol. 19, no. 33, Article ID 332001, 2008.
- R. A. Potyrailo, C. Surman, N. Nagraj, and A. Burns, “Materials and transducers toward selective wireless gas sensing,” Chemical Reviews, vol. 111, no. 11, pp. 7315–7354, 2011.
- M. E. Roberts, M. C. Lemieux, and Z. Bao, “Sorted and aligned single-walled carbon nanotube networks for transistor-based aqueous chemical sensors,” ACS Nano, vol. 3, no. 10, pp. 3287–3293, 2009.
- K. A. Mirica, J. M. Azzarelli, J. G. Weis, J. M. Schnorr, and T. M. Swager, “Rapid prototyping of carbon-based chemiresistive gas sensors on paper,” Proceedings of the National Academy of Sciences of the United States of America, vol. 110, no. 35, pp. E3265–E3270, 2013.
- J. Li, Y. Lu, Q. Ye, M. Cinke, J. Han, and M. Meyyappan, “Carbon nanotube sensors for gas and organic vapor detection,” Nano Letters, vol. 3, no. 7, pp. 929–933, 2003.
- J. Zhang, A. Boyd, A. Tselev, M. Paranjape, and P. Barbara, “Mechanism of NO2 detection in carbon nanotube field effect transistor chemical sensors,” Applied Physics Letters, vol. 88, no. 12, Article ID 123112, 2006.
- N. Peng, Q. Zhang, C. L. Chow, O. K. Tan, and N. Marzari, “Sensing mechanisms for carbon nanotube based NH3 gas detection,” Nano Letters, vol. 9, no. 4, pp. 1626–1630, 2009.
- J. Kong, M. G. Chapline, and H. Dai, “Functionalized Carbon Nanotubes for Molecular Hydrogen Sensors,” Advanced Materials, vol. 13, no. 18, pp. 1384–1386, 2001.
- K. Bradley, J.-C. P. Gabriel, A. Star, and G. Grüner, “Short-channel effects in contact-passivated nanotube chemical sensors,” Applied Physics Letters, vol. 83, no. 18, pp. 3821–3823, 2003.
- E. S. Snow and F. K. Perkins, “Capacitance and conductance of single-walled carbon nanotubes in the presence of chemical vapors,” Nano Letters, vol. 5, no. 12, pp. 2414–2417, 2005.
- E. S. Snow, F. K. Perkins, E. J. Houser, S. C. Badescu, and T. L. Reinecke, “Chemical detection with a single-walled carbon nanotube capacitor,” Science, vol. 307, no. 5717, pp. 1942–1945, 2005.
- J. Kong, N. R. Franklin, C. Zhou et al., “Nanotube molecular wires as chemical sensors,” Science, vol. 287, no. 5453, pp. 622–625, 2000.
- J. Kong and H. Dai, “Full and modulated chemical gating of individual carbon nanotubes by organic amine compounds,” Journal of Physical Chemistry B, vol. 105, no. 15, pp. 2890–2893, 2001.
- M. Grujicic, G. Cao, and R. Singh, “The effect of topological defects and oxygen adsorption on the electronic transport properties of single-walled carbon-nanotubes,” Applied Surface Science, vol. 211, no. 1–4, pp. 166–183, 2003.
- L. Valentini, F. Mercuri, I. Armentano et al., “Role of defects on the gas sensing properties of carbon nanotubes thin films: experiment and theory,” Chemical Physics Letters, vol. 387, no. 4–6, pp. 356–361, 2004.
- J. A. Robinson, E. S. Snow, Ş. C. Badescu, T. L. Reinecke, and F. K. Perkins, “Role of defects in single-walled carbon nanotube chemical sensors,” Nano Letters, vol. 6, no. 8, pp. 1747–1751, 2006.
- P. C. P. Watts, N. Mureau, Z. Tang, Y. Miyajima, J. David Carey, and S. R. P. Silva, “The importance of oxygen-containing defects on carbon nanotubes for the detection of polar and non-polar vapours through hydrogen bond formation,” Nanotechnology, vol. 18, no. 17, Article ID 175701, 2007.
- J. Zhang, H. Zou, Q. Qing et al., “Effect of chemical oxidation on the structure of single-walled carbon nanotubes,” Journal of Physical Chemistry B, vol. 107, no. 16, pp. 3712–3718, 2003.
- A. Felten, J. Ghijsen, J.-J. Pireaux et al., “Effect of oxygen rf-plasma on electronic properties of CNTs,” Journal of Physics D: Applied Physics, vol. 40, no. 23, pp. 7379–7382, 2007.
- A. Felten, C. Bittencourt, J. J. Pireaux, G. Van Lier, and J. C. Charlier, “Radio-frequency plasma functionalization of carbon nanotubes surface O2, NH3, and CF4 treatments,” Journal of Applied Physics, vol. 98, no. 7, Article ID 074308, 2005.
- J. H. Kim, M.-J. Song, C. J. Lee, J.-H. Lee, J.-H. Kim, and N. K. Min, “A comparative study of electrochemical and biointerfacial properties of acid- and plasma-treated single-walled carbon-nanotube-film electrode systems for use in biosensors,” Carbon, vol. 52, pp. 398–407, 2013.
- C. Wang, K. Takei, T. Takahashi, and A. Javey, “Carbon nanotube electronics—moving forward,” Chemical Society Reviews, vol. 42, no. 7, pp. 2592–2609, 2013.
- C. Wang, J. Zhang, and C. Zhou, “Macroelectronic integrated circuits using high-performance separated carbon nanotube thin-film transistors,” ACS Nano, vol. 4, no. 12, pp. 7123–7132, 2010.
- M. Engel, J. P. Small, M. Steiner et al., “Thin film nanotube transistors based on self-assembled, aligned, semiconducting carbon nanotube arrays,” ACS Nano, vol. 2, no. 12, pp. 2445–2452, 2008.
- N. Rouhi, D. Jain, and P. J. Burke, “High-performance semiconducting nanotube inks: progress and prospects,” ACS Nano, vol. 5, no. 11, pp. 8471–8487, 2011.
- C. Wang, J.-C. Chien, K. Takei et al., “Extremely bendable, high-performance integrated circuits using semiconducting carbon nanotube networks for digital, analog, and radio-frequency applications,” Nano Letters, vol. 12, no. 3, pp. 1527–1533, 2012.
- N. Rouhi, D. Jain, K. Zand, and P. J. Burke, “Fundamental limits on the mobility of nanotube-based semiconducting inks,” Advanced Materials, vol. 23, no. 1, pp. 94–99, 2011.
- K.-P. Yoo, K.-H. Kwon, N.-K. Min, M. J. Lee, and C. J. Lee, “Effects of O2 plasma treatment on NH3 sensing characteristics of multiwall carbon nanotube/polyaniline composite films,” Sensors and Actuators, B: Chemical, vol. 143, no. 1, pp. 333–340, 2009.
- A. Javey, J. Guo, Q. Wang, M. Lundstrom, and H. Dai, “Ballistic carbon nanotube field-effect transistors,” Nature, vol. 424, no. 6949, pp. 654–657, 2003.
- C. Lan, P. Srisungsitthisunti, P. B. Amama, T. S. Fisher, X. Xu, and R. G. Reifenberger, “Measurement of metal/carbon nanotube contact resistance by adjusting contact length using laser ablation,” Nanotechnology, vol. 19, no. 12, 2008.
- S. Li, Z. Yu, C. Rutherglen, and P. J. Burke, “Electrical properties of 0.4 cm long single-walled carbon nanotubes,” Nano Letters, vol. 4, no. 10, pp. 2003–2007, 2004.
- C. Wei, L. Dai, A. Roy, and T. B. Tolle, “Multifunctional chemical vapor sensors of aligned carbon nanotube and polymer composites,” Journal of the American Chemical Society, vol. 128, no. 5, pp. 1412-1413, 2006.
- F. Rigoni, S. Tognolini, P. Borghetti et al., “Enhancing the sensitivity of chemiresistor gas sensors based on pristine carbon nanotubes to detect low-ppb ammonia concentrations in the environment,” Analyst, vol. 138, no. 24, pp. 7392–7399, 2013.
- J. Zhao, H. Park, J. Han, and J. P. Lu, “Electronic properties of carbon nanotubes with covalent sidewall functionalization,” Journal of Physical Chemistry B, vol. 108, no. 14, pp. 4227–4230, 2004.
- J. Zhao, A. Buldum, J. Han, and J. P. Lu, “Gas molecule adsorption in carbon nanotubes and nanotube bundles,” Nanotechnology, vol. 13, no. 2, pp. 195–200, 2002.
- K. Bradley, J.-C. P. Gabriel, M. Briman, A. Star, and G. Grüner, “Charge transfer from ammonia physisorbed on nanotubes,” Physical Review Letters, vol. 91, no. 21, p. 218301, 2003.
- M. D. Ellison, M. J. Crotty, D. Koh, R. L. Spray, and K. E. Tate, “Adsorption of NH3 and NO2 on single-walled carbon nanotubes,” Journal of Physical Chemistry B, vol. 108, no. 23, pp. 7938–7943, 2004.
- J. Andzelm, N. Govind, and A. Maiti, “Nanotube-based gas sensors—role of structural defects,” Chemical Physics Letters, vol. 421, no. 1–3, pp. 58–62, 2006.
- K. G. Ong, K. Zeng, and C. A. Grimes, “A wireless, passive carbon nanotube-based gas sensor,” IEEE Sensors Journal, vol. 2, no. 2, pp. 82–88, 2002.
- J. H. Kim, J.-H. Jin, J.-Y. Lee, E. J. Park, and N. K. Min, “Covalent attachment of biomacromolecules to plasma-patterned and functionalized carbon nanotube-based devices for electrochemical biosensing,” Bioconjugate Chemistry, vol. 23, no. 10, pp. 2078–2086, 2012.
- A. Ricca and C. W. Bauschlicher Jr., “The adsorption of NO2 on (9,0) and (10,0) carbon nanotubes,” Chemical Physics, vol. 323, no. 2-3, pp. 511–518, 2006.
Copyright © 2017 Sung Joon Min 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.