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Nanotechnology and Nanomaterials » "Syntheses and Applications of Carbon Nanotubes and Their Composites", book edited by Satoru Suzuki , ISBN 978-953-51-1125-2, Published: May 9, 2013 under CC BY 3.0 license. © The Author(s).

Chapter 15

Latest Advances in Modified/Functionalized Carbon Nanotube- Based Gas Sensors

By Enid Contés-de Jesús, Jing Li and Carlos R. Cabrera
DOI: 10.5772/52173

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SWCNTs-sensor responses to (A) NO (10 – 200ppt) under in situ UV illumination, (B) NO2 (40 – 1000 ppt) under in situ UV illumination, (C) NH3 (5 – 500 ppm) without in situ UV illumination, and (D) NH3 (200 – 4000 ppt) under in situ UV illumination. (From Chen et al.  [40]. Copyright © 2012, with permission from Nature Publishing Group. )
Figure 1. SWCNTs-sensor responses to (A) NO (10 – 200ppt) under in situ UV illumination, (B) NO2 (40 – 1000 ppt) under in situ UV illumination, (C) NH3 (5 – 500 ppm) without in situ UV illumination, and (D) NH3 (200 – 4000 ppt) under in situ UV illumination. (From Chen et al. [40]. Copyright © 2012, with permission from Nature Publishing Group. )
Representation of the possible sensing mechanism of DMMP with TFQ functionalized SWCNTs. (From Wei et al.  [48]. Copyright © 2011, with permission from Institute of Physics Publishing. )
Figure 2. Representation of the possible sensing mechanism of DMMP with TFQ functionalized SWCNTs. (From Wei et al. [48]. Copyright © 2011, with permission from Institute of Physics Publishing. )
Responses of pristine (MC), oxygen plasma treated (O30) and fluorine plasma treated (F60) MWCNTs to 100-400 ppm of ethanol. (From Liu et al.  [52]Copyright © 2012, with permission from Elsevier. )
Figure 3. Responses of pristine (MC), oxygen plasma treated (O30) and fluorine plasma treated (F60) MWCNTs to 100-400 ppm of ethanol. (From Liu et al. [52]Copyright © 2012, with permission from Elsevier. )
Illustration of the steps to obtain oxyfluorinated CNTs modified with PANI. (From Yun et al. [68]. Copyright © 2012, with permission from Elsevier. )
Figure 4. Illustration of the steps to obtain oxyfluorinated CNTs modified with PANI. (From Yun et al. [68]. Copyright © 2012, with permission from Elsevier. )
A-D) Responses of the different Pd/DWCNTs composites when exposed to H2. (E) Calibration curves for the samples presented in figures (A-D). (From Rumiche et al.  [87] Copyright © 2012, with permission from Elsevier. )
Figure 5. A-D) Responses of the different Pd/DWCNTs composites when exposed to H2. (E) Calibration curves for the samples presented in figures (A-D). (From Rumiche et al. [87] Copyright © 2012, with permission from Elsevier. )
Response of SnO2/MWCNTs to NO2 at (A) room temperature and (B) 150 oC. (From Leghrib et al.  [64]. Copyright © 2010, with permission from Elsevier. )
Figure 6. Response of SnO2/MWCNTs to NO2 at (A) room temperature and (B) 150 oC. (From Leghrib et al. [64]. Copyright © 2010, with permission from Elsevier. )

Latest Advances in Modified/Functionalized Carbon Nanotube-Based Gas Sensors

Enid Contés-de Jesús1, Jing Li2 and Carlos R. Cabrera1

1. Introduction

A gas sensor is a device that when exposed to gaseous species, is able to alter one or more of its physical properties, so that can be measured and quantified, directly or indirectly. These devices are used for applications in homeland security, medical diagnosis, environmental pollution, food processing, industrial emission, public security, agriculture, aerospace and aeronautics, among others. Desirable characteristics of a gas sensor are selectivity for different gases, sensitivity at low concentrations, fast response, room temperature operation (some applications may require high temperature), low power consumption, low-cost, low maintenance and portability. Traditional techniques like gas chromatography (GC), GC coupled to mass spectrometry (GC-MS), Fourier transmission infrared spectroscopy (FTIR) and atomic emission detection (AED) provide high sensitivity, reliability and precision, but they are also bulky, time consuming, power consuming, operate at high temperature, and the high maintenance and requirement of trained technicians translate in high costs. In an effort to overcome those disadvantages, research in the area has been focused on the search for functional sensing materials.

Carbon nanotubes (CNTs) have been have been focus of intense research as alternative sensing material because of their attractive characteristics like chemical, thermal and mechanical stability, high surface area, metallic and semi-conductive properties and functionalization capability [1]. CNTs are graphene sheets rolled in a tubular fashion. Different types of CNTs can be synthesized: single walled carbon nanotubes (SWCNT), double wall carbon nanotubes (DWCNTs) and multi walled carbon nanotubes (MWCNT).

The publication of the first CNT-based sensor for NH3 and NO2 detection using an individual semiconducting SWCNT [2] triggered the research activity in this area. Pristine CNTs have shown to be chemically inactive to gas molecules in general. However, their modification/functionalization capability has been exploited throughout the last years, especially for the development of devices with enhanced selectivity and sensitivity for the room temperature detection of a wide variety of gases. Numerous articles and reviews focused on different aspect of CNTs-based sensors and summarizing their progress and potential have been published throughout the years. Some of them are listed in references [3-34]. A most recent review [35] addressing the technological and commercial aspects of CNTs sensors presents evidence of the continuous active research in the area and that they have real potential to complement or substitute current technologies.

This chapter presents a summary of selected original research articles that have been published between 2010 and present in which the main subject are modified/functionalized SWCNTs, DWCNTs and MWCNTs and their use as gas sensing material. The majority of the references included in this chapter content are based on experimental results. However, theoretical studies based on computational science are also included because of their importance in the study of CNT-based sensors. The use of different methods of calculations and simulation has been useful to design new structures and materials and to study, evaluate and predict the interactions and adsorption energies between those materials and gaseous molecules. First, we present current research activities on pristine CNTs-based sensors and the different approaches used to improve their sensitivity and selectivity without modifying the CNTs structure, followed by the review of CNTs modified with conducting polymers, metallic nanoparticles (NPs), nanostructured oxides and sidewall modification, doping and others. Different modification/functionalization techniques like chemical deposition, plasma, sputtering and electrodeposition are discussed. Gas sensors based on changes of electrical conductivity caused by adsorption of gas molecules (resistors) are the most common sensor type discussed in this review. Other sensing platforms like surface acoustic wave (SAW) and quartz microbalance (QMB)are also included.

2. Unmodified carbon nanotubes

Pristine CNTs are known for their high stability because of their strong sp2 carbon-carbon bonds and thus insensitive when used as sensing material for certain gases. However, the detection of NO, NO2 and NH3 has been previously reported. In order to improve their sensitivity and recovery time, different approaches like dispersion techniques to debundling the CNTs ropes, humidity assisted detection, application of an electric field, continuous use of ultraviolet (UV) light and even separation of semi-conductive types from conductive have been reported. The detection of NO, NO2 and NH3, as well as other gases like formaldehyde and dimethyl methylphosphonate (DMMP) with pristine SWCNTs are discussed in this section.

A MWCNTs based sensor was used for the detection of 50 ppm of nitrogen monoxide (NO) [36]. With the purpose to increase the sensitivity, an electric field was applied between two copper plates as electrodes, one of them containing MWCNTs-silicon wafer. It was found that when a positive potential was applied to the copper plate and the negative potential applied to the copper plate containing the MWCNTs-sensor, NO, being an electron acceptor, moves to the electron enriched zone, which is the one containing the MWCNTs-sensor and thus enhancement in the sensitivity is observed. The stronger the applied electric field, the better the sensitivity. However, applying a negative electric field was applied to the copper plate and a positive potential was applied to the copper plate containing the MWCNTs-sensor, the NO molecules moved away from the MWCNTs sensor and thus a decrease in the sensitivity is observed. The more negative the applied electric field, the lower the sensitivity of the sensor. Recovery of the sensors was achieved by applying reverse potential from the one used to perform the gas sensing experiments.

Cava, et al. proposed the use of a homogeneous film of MWCNTs prepared by the self-assembly technique and use it as an active layer for an oxygen gas sensor with increased sensitivity [37]. When the sensors were exposed to 10% O2 in Nitrogen at 160 oC, the electrical resistance decreased and showed a better oxygen sensitivity when compared to sensors prepared under the same condition but using the drop-cast method. The reason for this is that the self-assembly technique provides a better distribution of the nanotubes and thus promoting a better gas adsorption between nanotubes (inter-tube contact).

The high van der walls attraction between CNTs causes them to remain in bundles or agglomerated. This can represent a problem for their application as gas sensors because it results in less adsorption/interaction (binding) sites, which translates in less sensitivity. Considering this, different dispersion techniques were used by Ndiaye and coworkers for the preparation of CNTs based sensors for NO2 detection [38]. SWCNTs were dispersed in a surfactant, sodium dodecylbenzene sulfonate (NaDDBs) and an organic solvent, chloroform (CHCl3), drop-casted in IDEs and tested for the detection of 50, 100, 120, 200 ppb of NO2 at 80 oC. Sensors prepared with SWCNTs dispersed in NaDDBs showed better sensitivity than those with SWCNTs dispersed in chloroform. The explanation to this is that the surfactant was more effective in debundle the SWCNTs than the organic solvent. It was stated that even though the surfactant was not completely removed after several rinsing steps and heating treatment at 150oC, it does not have significant effect on the electronic behavior of the sensor. Both surfactant-dispersed and organic solvent-dispersed samples showed a decrease in resistance with increasing temperature, which demonstrate the semi-conductive behavior of the SWCNTs and thus no effect of the solvent.

A SWCNT-based gas sensor selective for NO2 and SO2 at room temperature and ambient pressure was developed by Yao et al. [39]. High sensitivity and selectivity for 2 ppm of each gas was achieved by controlling the humidity levels. For instance, at low humidity levels, the sensors showed to be selective for NO2and insensitive to SO2. At high humidity levels (92%), both gases were detected. However, NO2 showed a decrease in resistance and SO2 showed an increase in resistance.

Continuous in situ UV illumination on SWCNTs during gas sensing experiments was used to enhance the sensor’s overall performance in the detection of NO, NO2 and NH3 (Figure 1) [40]. Changes in conductance (∆G/G0) as function of time were recorded and used to prepare calibration curves in order to determine sensors sensitivity. It was found that the continuous exposure of the sensors to UV light under inert atmosphere (N2, Ar) regenerating the surface, therefore, enhances their sensitivity for the detection of NO and NO2. Linear responses were achieved at low concentrations and up to 50 ppm. Detection limits (DL), derived from the noise of the baseline and the slope obtained from the calibration curve, were found to be as low as 590 parts per quadrillion (ppq) and 1.51ppt for NO and NO2, respectively. For NH3 it was found not only that the in situ UV illumination reverses the direction of the changes in conductance, but it was also confirmed that it helps to improve the DL from 5.67 ppm to 27.8 ppt when tested under identical conditions. The achieved DL outperformed by several orders of magnitude the sensitivity of other CNTs-based NO, NO2and NH3 sensors that have been previously reported. This is attributed to the UV light inducing surface regeneration and actively removal of all gases adsorbed on SWCNTs surface. It is worth noticing that this in situ cleaning with continuous UV-light exposure without device degradation was just achieved under inert atmospheres.


Figure 1.

SWCNTs-sensor responses to (A) NO (10 – 200ppt) under in situ UV illumination, (B) NO2 (40 – 1000 ppt) under in situ UV illumination, (C) NH3 (5 – 500 ppm) without in situ UV illumination, and (D) NH3 (200 – 4000 ppt) under in situ UV illumination. (From Chen et al. [40]. Copyright © 2012, with permission from Nature Publishing Group. )

Battie and coworkers used sorted semi-conducting SWCNTs as sensing film for the detection of NO2 and NH3 [41]. The density gradient ultracentrifugation (DGU) technique was used to separate semi-conducting from as produced SWCNTs. Films of as produced and sorted semi-conducting SWCNTs were exposed to NO2 and NH3 in air. Both films showed decrease in resistance and increase in resistance as exposed to NO2 and NH3, respectively. Full recovery was achieved by applying heat after NH3 exposure and vacuum after NO2 exposure. However, semi-conducting SWCNTs films were more sensitive for NH3 than to NO2 at different concentrations at ppm level.

Horrillo et al. used SWCNTs films for the room temperature detection of Chemical Warfare Agents (CWA) [42]. Changes in resistance were measured as samples were exposed to simulants of CWA at different ppm levels, DL of 0.01 ppm, 0.1 ppm and 50 ppm were achieved for DMMP, dipropylene glycol methyl ether (DPGME) and dimethylacetamide (DMA), respectively. The most remarkable advantage is that the sensors perform better and at more sensitive at room temperature, when tested at different temperatures.

3. Surface modified carbon nanotubes

CNTS modified with different functional groups have been used for the development of sensors for detection of volatile organic compounds (VOCs) in the environment as well as in exhaled breath. For the detection of VOCs in air, Wang et al. worked in the preparation of a sensor array based on MWCNTs covalently modified with different functional groups like propargyl, allyl, alkyltriazole, thiochain, thioacid, hexafluoroisopropanol (HFIP) [43] and Shrisat, et al. reported another one based on SWCNTs modified with different porphyrins (organic macrocyclic compounds) likeoctaethyl porphyrin (OEP), ruthenium OEP (RuOEP), iron OEP (FeOEP), tetraphenylporphyrin (TPP), among others [44]. Penza et al. also worked in the modification of MWCNTs with TPP for the room temperature detection of VOCs [45]. In this case, the TTP contained two different metals, Zn (CNT:ZnTPP) and Mn (CNT:MnTPP). Sensors were exposed to ethanol, acetone, ethylacetate, toluene and Triethylamine at ppm levels and all showed increase in resistance when exposed to the different gases. CNT: MnTPP showed the highest sensitivity towards all gases with respect to unmodified CNTs but for triethylamine and CNT: ZnTPP was more sensitive to ethylacetate.

Two different CNT-based sensor arrays have been reported for the detection and pattern recognition of VOCs present in exhaled breath samples for medical diagnosis, Tisch et al. presented a sensor array containing different nanomaterials including organically functionalized random networks of SWCNTs for the detection of VOCs related to Parkinson disease and that were present in exhaled breath collected from rats [46]. Ionescu and coworkers reported a sensor array based on bilayers of SWCNTS and polycyclic aromatic hydrocarbons (PAH) for the detection of multiple sclerosis in exhaled human breath [47]. In general, the incorporation of organic functional groups provided not only enhanced sensitivity but also provided better selectivity for each gas when compared to pristine CNTs. The use of statistical techniques like principal component analysis (PCA), discriminant factor analysis (DFA) and linear discriminant analysis (LDA) was possible to determine the discrimination capability of the sensors toward each VOC.

SWCNTs were functionalized with tetrafluorohydroquinone (TFQ) at the room temperature for detection of dimethyl methylphosponate (DMMP) at parts per trillion (ppt) levels (Figure 2) [48]. The conductance of the TFQ-SWCNTs samples increased as function of concentration when exposed to DMMP in N2 in a concentration range from 20ppt to 5.4ppb. Sensors showed fast response and ultra sensitivity down to 20ppt when compared to unmodified SWCNTs sensor, which had a DL of nearly 1 ppm. The presence of TFQ clearly showed to improve the sensitivity and this is because it provides additional binding sites thru hydrogen bonds between hydroxyl groups in TQF and DMMP. In addition, TQF tailors the electronic properties of SWCNTs via hole doping.


Figure 2.

Representation of the possible sensing mechanism of DMMP with TFQ functionalized SWCNTs. (From Wei et al. [48]. Copyright © 2011, with permission from Institute of Physics Publishing. )

Wang et al. deposited a uniform network of SWCNT with carboxylic groups (-COOH) on a flexible poly (dimethyldiallylammonium chloride) (PDDA) modified polyimide (PI) substrate for DMMP detection at room temperature [49]. Changes in resistance as function of time were measured as the sensors were exposed to DMMP in N2 at a concentration range of 1-40 ppm. Calibration curve showed a [17] linear increase of resistance as function of concentration and responses were found to be fast, stable and reproducible. Sensors showed to be selective to DMMP in presence of other volatile organic vapors like methanol, xylene and hexane, among others. Changing the carrier gas from N2 to air caused the responses to DMMP to be lower which might be due to influence of oxygen and humidity contained in air. The apparent enhanced performance of this SWCNTs (-COOH) flexible sensor when compared to sensors prepared on Si/SiO2 rigid substrates is attributed to the presence of PDDA, which is a polymer that absorbs DMMP. There is no information on the adsorption of DMMP by PDDA and its possible effect in the recovery of the sensors.

MWCNTs were oxidized with KMnO4 to add oxygenated functional groups, mainly (-COOH) for the detection of organic vapors [50]. Oxidized MWCNTs in form of a bucky paper were exposed to different concentrations of acetone. Variations in electrical resistance were recorded for both unmodified and oxidized MWCNTs. Oxidized MWCNTs showed higher sensitivity to acetone (2.3 vol. %) than unmodified ones, and good selectivity when sensing other oxygen containing vapors such as diethyl ether and methanol. The sensors also showed complete reversibility and high reproducibility for all tested vapors.

MWCNTs were chemically treated with acid to obtain hydroxyl groups (OH) and used as sensing material for humidity sensors [51]. Changes in resistance were measured as the RH was varied from 11% to 98%. It was observed that the resistance increased as sensors were exposed to the different humidity levels. It was found that acid treated SWCNTS were more sensitive to humidity than pristine MWCNTs. The higher sensitivity of Acid treated SWCNTs is attributed to their higher surface and thus more adsorption sites that result from the acid treatment. Sensors showed fast response and to be stable. As with most humidity sensors, the recovery time was longer than response time due to slow desorption of water molecules.

Purified MWCNTs were treated with oxygen plasma or fluorine plasma and used for the detection of ethanol (Figure 3) [52]. Changes in resistance as function of time were recorded for the sensors when exposed of 50-500 ppm of ethanol vapor in air. Samples treated with oxygen plasma for 30 sec and with fluorine plasma for 60 sec showed the highest sensitivity to 100 ppm of ethanol, compared to pristine MWCNTS and other oxygen and fluorine plasma treated for different duration time. However, fluorine plasma treated samples showed the better sensitivity and reduced response and recovery time. The improvement of the fluorine plasma treated samples is explained by the difference in electronegativity between oxygen and fluorine.


Figure 3.

Responses of pristine (MC), oxygen plasma treated (O30) and fluorine plasma treated (F60) MWCNTs to 100-400 ppm of ethanol. (From Liu et al. [52]Copyright © 2012, with permission from Elsevier. )

Thermally fluorinated MWCNTs (TFC) were used for NO gas detection at room temperature [53]. The effect of thermal fluorination process was performed at various temperatures (100 -1000 oC) and 200 oC was found to be the optimum fluorination temperature. TFC samples prepared at temperatures higher than 200 oC showed a decrease of the fluorine functional groups, and even fluorine-assisted pyrolysis and fluorine-induced reorientation of the MWCNTs structure occurred at 1000 oC. TFC prepared at 200 oC showed high sensitivity, stability, reproducibility and full recovery, when their gas sensing properties were evaluated towards the detection of 50 ppm NO in dry air. Interestingly, the presence of fluorine reverses the electron transfer process, when compared to pristine MWCNTs, allowing them to go from NO to MWCNTs and thus causing an increase in resistance. The fluorination not only helped to enhance the sensitivity but also made the sensors insensitive to humidity changes.

MWCNTs were modified with amino groups for the detection of formaldehyde at ppb level [54]. Changes in resistance as function of time were measured as the sensors were exposed to formaldehyde in a concentration range between 20 and 200 ppb. Sensors containing MWCNTs with higher amino group content (18%) were 2.4 and 13 times more sensitive to formaldehyde than samples containing 5% amino groups and pristine CNTs, respectively. Short response times are due to a chemical reaction between the aldehyde and amino group. For the same reason, the recovery times are longer, since chemical desorption is a slow and irreversible process. SWCNTs with 18% amino groups showed to be selective to formaldehyde when tested against interferences like acetone, CO2, ammonia, methanol and ethanol.

Silicon (Si) nitrogen (N), and phosphorous-nitrogen (P-N) were used to modify MWCNTs and study their gas sensing properties for hydrogen peroxide, sodium hypochlorite and1, 2-dichloromethane, nitrogen, and ammonia [55]. Samples of Si-MWCNTs, N-SWCNTs, and P-N-SWCNTs were prepared by aerosol chemical vapor deposition. It is known that the incorporation of heteroatoms in the CNT structure changes its morphology and thus the reactivity. To evaluate the gas sensing properties of the prepared materials, changes in resistance as function of time were recorded when they were exposed to the different gases. Exposure to N2 caused the removal of physisorbed water molecules and thus a decrease in the resistance values. Sodium hypochlorite and dichloroethane caused decrease in resistance of pristine MWCNTs and Si-MWCNTs due to charge transfer (electrons) from CNTs to Chlorine atoms and increase in resistance of N-P MWCNTs. Ammonia showed the opposite effect in resistance. These results demonstrate the p-type semiconductor behavior for pristine MWCNTs and Si-MWCNTs and n-type of N-MWCNTs and N-P-MWCNTs. All sensors recovered in 10 min for all gases with the exception of ammonia that exceeded 1 hour.

In an effort to enhance the selectivity of SWCNTs-based vapor sensors, Battie et al. worked in the preparation of SWCNTs covered with a mesoporous silica film [56]. Sensors were fabricated by covering a SWCNTs film with a mesoporous silica film via by sol-gel deposition technique. Characterization of the sensors was done by measuring changes in resistance when exposed to 200 ppm of NO2, NH3, and H2O in dry air. A sensor of SWCNTs without the mesoporous silica film prepared and tested under the same conditions. While the SWCNTs sensor showed to be sensitive to the three gases, the sensor based on SWCNTs film covered with mesoporous silica film showed to insensitivity to H2O, and its sensitivity for NH3 was considerably reduced. These observations can be explained considering the polarization capabilities and dipole moments of the silanol groups contained in the mesoporous silica layer and the gas molecules. The silanol groups allow the mesoporous silica film to act as a diffusion barrier and allow the physical interaction and entrapment of highly polarized molecules like H2O and NH3, avoiding them to get in contact with the SWCNTs layer. On the other hand, the sensitivity to NO2 was greatly enhanced, compared to the SWCNTs sensor. Compared to H2O and NH3, NO2 has a weaker dipole moment and its diffusion thru the mesoporous silica gel and to the SWCNTs film results easier and thus its enhanced and selective detection.

Computational studies based on SWCNTs doped with heteroatoms have been also reported. Ab initio (ABINIT) simulations of CNTs doped with heteroatoms like boron, oxygen and nitrogen were performed to predict the behavior of the doped CNTs and to study their application as gas sensors for Cl2, CO, NO and H2 [57, 58]. Density functional theory (DFT) applied in the ABINIT code and the Generalized Gradient Approximation (GGA) were used to perform the calculations. The calculations demonstrated that doping the CNTs with B, O, and N causes a shift in the conduction band of the CNTs. For B and O, the conduction band shifts downward and creates a p-type semiconducting material. On the other hand, N dopant causes the conduction band to shift upward and create an n-type semiconducting material. Calculations also demonstrated that Cl2, NO, H2and CO considerably affects the NTs density of states (DOS) and Fermi level as the gases become close to their surface. B-doped CNTs can detect CO, NO and H2 gas molecules, O-doped can detect H2, Cl2 and CO and N-doped can detect CO, NO and Cl2.

Similarly, Hamadanian et al. presented a computational study of Al-substituted SWCNTs (10, 0) (2.5% and 25%) and their use as CO gas sensor [59]. DFT calculations (local density approximation with ultrasoft pseudopotential) were used to study the electronic properties of Al-substituted SWCNTs and how those properties are affected by the adsorption of CO molecules. Substitution of one carbon atom with an Al atom causes deformation of the 6-membered ring and increasing the bond length. Doping with Al also alters the DOS and band structure of the CNTs. Since Al has one electron less than C in the valence shell, introduces one electron holes in the band structure, therefore the tube is changed to p-type semiconductor. Calculations showed low adsorption energy for CO on pristine CNTs and that CO does not cause significant changes in the electronic band structure and DOS when adsorbed on pristine CNTs. These results confirm that pristine CNTs are insensitive to CO as result of their weak physical interaction. When CO is adsorbed on both 2.5% and 25% Al-substituted SWCNTs, it causes severe changes in the Band structure near Fermi level. Those changes strongly depended on the site of CNTs and the direction in which the CO molecule interacts. For instance, the most stable adsorption structure is when the C of the CO interacts with the middle point of a C-C bond of CNTs. Even when the adsorption energies of CO in 25% Al-substituted SWCNTs were higher than in 5% Al-substituted SWCNTs, the fact that the conductivity of the proposed material changes, makes them suitable for their use as CO gas sensing material.

Metal oxide Nanotube Type Op T. oC Target (gas) DL Response Time Ref.
Co3O4 SWNTsRT, 250NOx 20ppmNS[61]
H2 4%
SnO2 SWNTs200NO2 2ppmNS[63]
SnO2 MWNTsRT, 150NO2 1ppm3min (150C)
4min (RT)
WO3 MWNTs350H2 100ppm*Ns[65]
SnO2 MWNTs320Ethanol[66]
SnO2 O-dopedRTNO2 100ppb7min[67]

Table 1.

Summary of metal oxide NPs used to modify CNTs for gas sensor applications.

[i] - *Lowest tested concentration

4. Conducting polymers and CNT composites

Conducting polymers have been widely used to enhance the sensing properties of CNTs-based sensors. CNTs unique characteristics combined with polymer’s delocalized bonds, high permeability and low density have demonstrated that it is possible to detect many different gases with high sensitivity, fast response and good reproducibility. Previous reports on polymer/CNTs-based sensor have been summarized and reviewed [7-9, 12]. However, some challenges to overcome are aggregation or agglomeration of CNTs, thermal stability and selectivity, among others. Polymer/CNTs composites used in resistors, SAW and QMB type of sensors are discussed.

CNTs were used to improve Polyaniline (PANi) poor thermal stability (Figure 4) [68]. The proposed solution to this was the uniform incorporation of CNTs in the polymer network. Considering that one of the problems of MWCNTs is their aggregation and agglomeration, they were oxyfluorinated under different conditions in order to obtain a better dispersion in aqueous solution and it was found that the better dispersion was obtained with the MWCNTs with the highest oxygen content. The oxyfluorinated MWCNTs were then mixed with aniline and ammonium persulfate (APS) and other chemicals, for in-situ polymerization. Changes in resistance as function of time were used to characterize and evaluate the resulting PANi/MWCNTs composite was for the detection of ammonia (NH3) in a concentration range of 1-50 ppm. PANi/MWCNTs composite with the highest oxygen content had a uniform composition, improved thermal stability and highest and faster response for 50 ppm of NH3. The composite was able to detect 1 ppm and showed excellent repeatability for cycling exposures to 50 ppm and it needed heat treatment to accelerate the NH3 desorption and thus the recovery of the sensor. A possible drawback is the selectivity to NH3 among gases that can extract protons (H+) from PANi.


Figure 4.

Illustration of the steps to obtain oxyfluorinated CNTs modified with PANI. (From Yun et al. [68]. Copyright © 2012, with permission from Elsevier. )

Mangu et al. also worked in the preparation of PANi-MCNTs as well as Poly (3, 4-ethylenedioxythiophene) poly (styrenesulfonate) (PEDOT:PSS)-MWCNTs composites for the detection of 100 ppm of NO2 and NH3 [69]. This group studied the effect of dissolving the polymers in different solvents for the gas sensing properties. PANi was dissolved in dimethyl sulfoxide (DMSO), N, N-dimethyl formamide (DMF), ethylene glycol (EG) and 2-propanol. PEDOT: PSS was dissolved in DMSO, DMF and 0.1M sodium hydroxide (NaOH). Each polymer solution was spin-coated in plasma treated MWCNTs and evaluated as sensing material. All PANi-MWCNTs composited showed an increase in resistance for NH3 and a decrease in resistance for NO2, which is typical of p-type semiconducting composite films. All PANi-MWCNTs composites were selective to NO2. However, better sensitivities were achieved when PANi was dissolved in 2-propanol and DMSO for NH3 and for NO2, respectively. On the other hand, all PEDOT:PSS-MWCNTs composites were also excellent for the detection if both NO2 and NH3. PEDOT: PSS-MWCNTs (prepared without any solvent) showed to be more sensitive to NH3 and PEDOT:PSS dissolved in NaOH to NO2.

Sayago, et al. have worked on the preparation of different composites using polymers with small percentages of CNTs as sensitive layers for surface acoustic wave (SAW) gas sensors [70-72]. Composites of polyisobutilene (PIB), polyepichlorohydrin (PECH) and polyetherurethane (PEUT) with 2% and 5% of MWCNTs were prepared and used to detect volatile organic compounds (VOCs) at room temperature using SAW-sensor arrays. All the samples showed responses (frequency shifts) for octane and toluene (25-200 ppm), even though some samples were more sensitive than the others. For instance, samples with PIB/5%MWCNTs showed higher sensitivity for octane while PECH/2%MWCNTs and PEUT/2%MWCNTs were more sensitive to toluene. The difference in sensitivity is attributed to the difference in affinity between polymers and VOCs due to their respective polarities. The detection and recovery times were fast and fully reversible, which means that the main interaction is physisorption. The role of the MWCNTs is unknown. In general, their presence in the composite showed to improve sensitivity and reduce the limits of detection (LOD) but did not affect selectivity, response and recovery times.

Another SAW gas sensor was reported by Viespe et al. for the detection of methanol, ethanol, toluene using different polyethyleneimine (PEI)-based nanocomposite as sensitive layer, including MWCNTs-PEI [73]. In general, frequency shifts were proportional to the gas concentration and MWCNTs-PEI sensors showed better response time and higher sensitivity than the PEI-sensor. However, it did not show the best LOD when compared to the other PEI-based nanocomposite. The MWCNTs-PEI sensors showed higher sensitivity towards toluene and lower sensitivity to methanol when compared to ethanol.

Biopolymer/CNTs composites for chemical vapor sensors were produced by using two different biopolymers, cellulose, the most naturally abundant one and poly (lactic acid) (PLA). Considering that previous studies have shown that a homogeneous distribution of MCNTs in the cellulose matrix can improve the polymer’s mechanical and electrical characteristics, MWCNTs were functionalized with imidazolide groups and covalently attached it to cellulose chains [74]. The resulting material, a paper-like film, was then used as sensing element for the detection of methanol, ethanol, 1-propanol and 1-butanol at ppm levels. Responses were measured by changes in resistance and were found to be reversible and consistent for all the tested vapors. However, the sensor only showed linear responses as function of concentration for 1-propanol in the range of 400-3600 ppm. The other composite, PLA/MWCNTs was prepared by doping the biopolymer with2 and 5% of MWCNTs and annealing, in order to understand the effect of MWCNTs in the crystallinity of the polymer and its performance in the detection of toluene, water, methanol and chloroform [75]. PLA/2%-MWCNTs showed highest responses for all gases, when compared to PLA/3%-MWCNTs. However, it was found that all samples were selective to chloroform. Moreover, annealing the samples showed a decrease in the responses that were significantly lower than the untreated ones. Annealing did not affect the selectivity to chloroform but it considerably affected its sensitivity.

Plasma-treated MWCNTs (p-MWCNTs) polyimide (PI) composite films (p-MWCNTs-PI) were developed by Yoo et al. in an effort to overcome some of the problems presented by PI-based resistive-type sensors, e. g. nonlinear sensitivity to relative humidity [33]. When tested as sensing material for 10-95% relative humidity (RH), p-MWCNTs-PI showed better sensitivity and linear response (resistance) as function of humidity, when compared to pristine-MWCNT-PI and pristine PI. The increase of p-MWCNTs content inp-MWCNTs-PI films not only showed improved the linearity and sensitivity but also lower resistance values. Lower resistance values might improve the performance at low RH range, a problem that PI resistive-type sensors present because of their high resistance values.

Yuana and coworkers prepared a sensor array based on polymer/MWCNTs composites for the selective detection of chloroform (CHCl3), tetrahydrofuran (THF) and methanol (MeOH) [76]. Ethyl cellulose (EC), poly [methyl vinyl ether-alt-maleic acid] (PMVEMA), hydroxypropyl methyl cellulose (HPMC), poly (alpha-methylstyrene) (PMS), poly (vinyl benzyl chloride) (PVBC) and poly (ethyleneadipate) (PEA) were the polymers used to prepare the polymer/MWCNTs composites and to provide uniqueness to each sensor in terms of their physical and chemical characteristics like molecular structure, polymer length, polarity and intermolecular forces. Changes in resistance as function of time were recorded for the sensor array when exposed to the different gases at different temperatures (30 40, 50, 60 oC) and 50-60% R. H. The sensors showed to be selective to the three gases at the different temperatures when in presence of vapor molecules of chloride, cyclic oxide and hydroxide groups. The decreasing order of sensitivity concurred with the order of decreasing conductivity: PEA/MWCNTs >EC/MWCNTs >PMVEMA/MWCNTs >PVBC/MWCNTs >HPMC/MWCNTs >PMS/MWCNTs.

SWCNTs modified with Poly- (D) glucosamine (Chitosan) (SWCNTs-CHIT) were as high performance hydrogen sensor [77]. Three types of sensors were prepared: SWCNTs deposited on glass substrate (type 1), SWCNTs deposited over a glass substrate modified with CHIT-film (type 2), Chit-film deposited over SWCNTs deposited over a glass substrate. Each type of sensor showed a different changes in resistance when exposed to 4% H2 in air. Increase in resistance was observed for three types of sensors and good recovery but for type (3) sensor. Sensors modified with CHIT showed better sensitivity. Moreover, the authors explained that the improved sensitivity was far higher than that reported for Pd-SWCNTs based sensors, which are commonly used for H2 detection. The enhanced performance of SWCNTs-CHIT can be explained by the strong interaction/ binding of the H2 molecules with/to the –OH and –NH3 groups contained in CHIT, which also explains the poor recovery of type 3 sensor.

SWCNTs were modified with Polypyrrole (PPy) and 5, 10, 15, 20-tetraphenylporphyrine (TPP) to prepare composites for the detection of 1-butanol in nitrogen using a quartz microbalance (QMB) [78]. The QMB gold electrodes were coated with PPy/SWCNTs-COOH, PPy/SWCNTs-COOH/SWCNTs-TPP via electropolymerization. Frequency shifts of the quartz crystal resonator as function of time were measured for the sensors when exposed to 1-butanol in ppb concentration range. Even though both composites showed good and higher response magnitudes than QMB prepared with other composites that did not contain CNTs, PPy/SWCNTs-COOH/SWCNTs-TPP showed better performance than PPy/SWCNTs-COOH. The results demonstrate that the incorporation of CNTs enhanced the sensitivity towards the detection of 1-butanol.

Lu et al. reported a sensor array containing pristine SWCNTs, Rh-loaded SWCNTs, PEI/SWCNTs and other CNTs with different coatings and loadings for the detection of hydrogen peroxide (H2O2) [79]. The measurements of changes in resistance as function of time were used to analyze the sensor array performance when exposed to H2O2. Pristine SWCNTs showed strong increases in resistance and fast responses for H2O2 and an estimated DL (by IUPAC definition) of 25 ppm. But when the sensor array was exposed to H2O and CH3OH in order to test its selectivity, pristine SWCNTs showed also good responses for both chemicals, which means that the discrimination capabilities towards H2O2 are limited. On the other hand, the PEI/SWCNTs sensors were sensitive to H2O2, showing decreases in resistance for each exposure. The PEI/SWCNTs did not show significant changes in resistance when exposed to H2O and CH3OH, which makes it selective to H2O2 under the tested conditions.

Polymer CNT Type Sensor
Target DL Ref.
PECH, PEUT, PIBMWCNTsSAWToluene1.7-12.2ppm[70 72]
PANiMWCNTsResistorNH3 1ppm[68]
PEDOT:PSSMWCNTsResistorNH3 100ppm*[69]
CHISWCNTsResistorH2 4%*[77]
ECMWCNTsResistorTHF, CH3Cl2, MeOHNS[76]
PEISWCNTsresistorH2O2 NS[79 80]

Table 2.

Summary of polymers used for the preparation of polymer/CNTs-based sensors.

[i] - * Lowest detected concentration

[ii] -

5. Metal nanoparticlesdecorated CNTs

Electronic, physical and chemical properties of metallic nanoclusters are usually sensitive to the changes in environment [81]. CNTs decorated with metallic nanoparticles (NPs) have been widely used to achieve selectivity and improve the sensitivity, response time and DLs for a variety of gas detections. Layer by layer, electrodeposition, chemical deposition, electrochemical deposition and sputtering are the methods used to prepare the metallic NP-CNTs composites discussed in this section.

SWCNTs films were modified with Pd NPs using sputtering method [82]. After apply different deposition times (40 – 160 s), it was found that 120 s was the optimum deposition time to obtain enhanced sensor response for 1% H2 in dry air at 50 oC. A typical response curve (igas/iair vs. time) showed differences in response and recovery between the first and following H2 sensing cycles. FTIR studies were used to support and explain those differences and mechanisms of detection. The first cycle showed an overall larger electrical current in the presence of H2and then it reached a new steady state. When the atmosphere was change to dry air, the current did not go to its original value but remained in the steady state, which is considered as an irreversible response. The explanation to this is that is atomized by the Pd NPs and spilled to the surface of the MWCNTs, occurring the chemical and irreversible reaction of hydrogenation of the carbonyl groups of the MWCNTs at the first cycle. The second cycle and following ones started at the steady state where the first cycle finished and the electrical current showed a decrease in the presence of H2 and when the atmosphere was changed to dry air, the electrical current recovered back to where the cycle started. This reversible behavior is explained as physisorption of H2 molecules onto Pd/SWCNTs.

Pd/MWCNTs and Pt-Pd/MWCNTs composites were tested for the detection of H2 in a concentration range of 20 ppm– 2% in N2 and 200 ppm – 2% in air [83]. Composites were prepared by growing CNTs yarns and then covered them with a layer of Pd NPs or sequentially deposited layers of Pd and Pt NPs, using a recently developed technique called self-fuelled electrodeposition (SFED). Exposure to 1% H2using N2 with 1% air as carrier gas. As with other Pd/CNTs-based sensors [82], an initial irreversible drop in resistance was observed, and after that, the sensor reached a steady state. A stable baseline was established just after a couple of exposure/recovery cycles. Pd-MWCNTs was not able to detect H2 concentrations below 20 ppm but with the Pt-Pd/MWCNTs composites it was possible to detect concentrations as small as 5 ppm (0.0005%). The sensor saturated at 100 ppm and higher concentrations. When the same experiments were performed using air as carrier gas, it was found that the detection limit for both composites decreased.

A Pd/MWCNTs flexible substrate H2 sensor was fabricated using the layer-by-layer technique [84]. For this, an Au IDE was sputtered over a polyester (PET) film, followed by the fabrication of a poly (4-styrenesulfonic acid-co-maleic acid)/poly (allylamine hydrochloride) (PSSMA/PAH) bilayer film. Then, a MWCNTs layer was deposited over the PSSMA/PAH bilayer film and decorated with Pd NPs using chemical deposition. The sensors were exposed to H2 in a range of concentrations between 200 and 40000 ppm at room temperature and 53% RH. The rapid response and higher sensitivity of the Pd/MWCNTs when compared to plain MWCNTs is attributed to the well known catalytic effect of Pd NPs. Because the detection mechanism is the dissociation of the H2 molecules on the surface of the Pd NPs, the linear relation was found to be between the sensor’s response and the square root of the concentration. It also showed to be selective to H2 at concentrations higher than 1000 ppm (vs. NH3, CO, CH4 and others), to be highly reproducible, to have long-term stability and comparable to similar sensors fabricated in rigid substrates.

Zilli et al. demonstrated that the H2sensing capacity of the Pd/MWCNTs nanocomposite is affected by the different stages of purification of the CNTs [85]. Pd NPs were chemically deposited on pristine MWCNTs (Pd-CNT-P), gas-phase oxidized MWCNTs (Pd-CNT-O) and gas-phase oxidized/acid treated MWCNTs (Pd-CNT-A) and used as H2 sensing material. All three nanocomposites showed increase in resistance as function of time in the presence of 500µL (STP) of H2 and an immediate decrease when the H2 disappeared from the testing chamber. However, Pd-CNT-O showed to be more sensitive than Pd-CNT-P and Pd-CNT-A, which both showed similar responses. The reason for these results is that for CNT-P, catalytic Fe NPs, used for the CNT growth, are encapsulated inside the CNTs and in CNT-A, the Fe NPs were removed the during the acid treatment. After the gas-phase oxidation process (CNT-O), the Fe NPs become exposed and at the same time, oxygen-containing groups are formed in the surface of CNTs, which act as additional anchoring site for Pd NPs and thus making the Pd-CNT-O sample more sensitive to H2.

Pd/SWCNT composites were prepared by using a poly (amido amine) (PAMAM) dendrimer assisted synthesis, followed by a pyrolysis step to remove the dendrimers [86]. For H2 sensing experiments, the samples were deposited over Ti/Au electrodes and changes in resistance as function of time were measured. The Pd/SWCNTs samples showed to be more sensitive to 10, 000 ppm of H2 at room temperature, when compared to samples of chemically reduced Pd on SWCNTs (without the presence of dendrimer) and Pd/PAMAM-SWCNTs. Moreover, these samples were able to detect all of the concentrations in a 10-100 ppm range. It was concluded that not only the dendrimers provided more nucleation sites for the Pd NPs and thus higher NPs density, but also that the removal of the dendrimers thru the pyrolysis step reduces the distance between the NPs and the SWCNTs and consequently reduces the delay in electron transfer, allowing faster response times.

Double wall carbon nanotubes (DWCNTs) have shown to have longer length, compared to SWNTs, provide a better percolation behavior, the possibility of modifying the outer layer without modifying the inner one and flexibility are some of their attractive characteristics. Considering those characteristics, Rumiche et al. evaluated Pd NPs/ (DWCNTs) composites as room temperature H2 sensor (Figure 5) [87]. Different amounts of DWNTs (15 and 20 µL) were deposited over silicon oxide substrates and decorated with 1, 3 and 6nm layers of Pd NPs. To evaluate their sensing properties, changes in resistance as function of time were recorded when exposed to 3%, 2%, 1%, 0.5%, 0.3%, 0.2%, 0.1%, and 0.05% of H2 in dry air. Samples containing 1nm Pd layer were unsuccessful detecting any of the tested concentrations. On the other hand, samples containing 3 and 6nm Pd layer showed overall similar performance in terms of increases of resistance and recovery. When analyzing the results for the lowest tested H2 concentration (0.05%)it was found that the increase in resistance was comparable for samples with same Pd layer thickness and different DWCNTs content (e. g. 3nm thick Pd layer deposited over 15µL DWCNTs was comparable to of 3nm thick Pd layer over 20µL DWCNTs). However, the increase in Pd coating thickness produced a reduction in the response. The obtained results confirmed that the combination of the amount of DWCNTs and the Pd-layer thickness directly affects the sensitivity of the sensors.

Another H2 sensor based on N-doped MWCNTs electrochemically decorated with Au NPs (Au-NMWCNTs) was presented by Sadek and collaborators [88]. N-doped MWCNTs were chosen because they have enhanced surface reactivity and chemically active sites for the nucleation of Au NPs during the electrodeposition process. NPs of different sizes were obtained with variation of electrodeposition potential. Changes in resistance as function of time were used to evaluate the performance of the Au-NMWCNTs sensors when exposed to different H2 concentration between 0.06% and 1%. Sensitivity, response time and recovery time highly depended on the size of the AuNPs: the smallest the size the better the sensitivity and the shorter the response and recovery times.

Penza et al. worked in the modification of SWCNTs with Pt, Ru and NiNPs to monitor toxic, landfill, and greenhouse gases (CO2, CH4, NH3, and NO2) [89, 90]. Pt NP layers with thickness of 8, 15 and 30 nm were sputtered over SWCNTs films and exposed to the different gases at an operation temperature of 120oC. Changes in resistance as function of time showed that Pt-SWCNTs had better sensitivity than unmodified SWCNTs. It was also found that the sensitivity depended on the layer thickness. For instance, 8 nm Pt layer-SWCNTs showed highest sensitivity for NO2 and CH4 and 15 nm Pt layer-SWCNTs showed better sensitivity for NH3 and CO2. In a similar study, a sensor array containing Pt, Ru, and Ag NPs sputtered over SWCNTs with a thickness of 5nmwas able to detect and selectively discriminate between landfill gases. Concentrations as low as 100 ppb of NO2 were selectively detected at a temperature of 120 oC.


Figure 5.

A-D) Responses of the different Pd/DWCNTs composites when exposed to H2. (E) Calibration curves for the samples presented in figures (A-D). (From Rumiche et al. [87] Copyright © 2012, with permission from Elsevier. )

Lu et al. used pristine SWCNTs, fluorinated SWCNTs (F-SWCNTs) and rhodium doped SWCNTs (Rh-SWCNTs) and other various coatings and dopings on the SWCNTs for the room temperature detection of formaldehyde (HCOH) [80]. The measurements of changes in resistance as function of time when the array was exposed to the different concentrations of formaldehyde were used to analyze the sensor array performance. When exposed to 0.71 ppm formaldehyde, pristine SWCNTs showed the higher response, followed by Rh/SWCNTs and F-SWCNTs, which were less sensitive. The other CNTs with different coating and loadings were insensitive to formaldehyde. However, when the array was exposed to formaldehyde at concentrations as low as 0.01 ppm (10ppb), Rh/SWCNTs sensor showed to be more sensitive and the presented an estimated DL (by IUPAC definition) of 10ppb. The DL for pristine SWCNTs and F-SWCNTs sensors were 15ppb and 20ppb, respectively. The three sensors presented very fast response (~18sec) and recovery time of approximately 1 minute.

Theoretical studies have been used to study the interaction between Pd and Pt NPs decoratedCNTs and a wide variety of gases for different applications. Zhou et al. used the density functional theory (DFT) to study the adsorption and interaction of SO2, CH3OH, and CH4 with Pd-SWCNTs [91]. The replacement of a central C atom of the CNTs with a Pd atom causes structural deformations. As SO2 is adsorbed, there is a charge transfer from Pd-SWCNT to SO2. As for CH3OH, the appropriate adsorption conformation is thru the lone par of the oxygen of CH3OH and thus occurring an overall charge transfer from CH3OH to Pd-SWCNT. The interaction between Pd-SWCNT and CH4 is similar in that the charge transfer occurs from Pd-SWCNT to the gas. However, the interaction between Pd-SWCNTs and CH4 is not as strong as the interaction between Pd-SWCNT and SO2 or even CH3OH.

NPNT TypeTarget Sensor
PdMWCNTH2 Resistor1%[82]
PdMWCNTsH2 Resistor10000ppm*[84]
PdMWCNTsH2 ResistorNS[85]
Pd-PtMWCNTsH2 Resistor5ppm[83]
PdSWCNTsH2 Resistor10ppm[86]
PdDWCNTsH2 Resistor0.05[87]
Pt, Ru, AgSWCNTsCO2,CH4, NH3,NO2 Resistor100ppb NO2 [89 , 90]
AuN-doped MWCNTsH2 Resistor0.06%*[88]

Table 3.

Metallic nanoparticles used to decorate SWCNTs for gas sensing applications

[i] - *Tested concentration

[ii] - ^For concentrations >1%

Li and co workers investigated the adsorption of CO and NO on SWCNTs-decorated with Pd and Pt using first-principle calculations [92]. It was found that the electronic properties of SWCNTs change upon modification with Pd or Pd atoms. The semi-conductive band gap is decreased compared to pristine SWCNTs. The reason for the observed decrease in the band gap is due to charge transfer from the Pd and Pt atoms to the surface of the SWCNTs. Different from pristine SWCNT that show poor adsorption, Pd-SWCNTs and Pt-SWCNTs showed to chemisorb CO molecules as well as NO. However, Pt-SWCNTs showed bigger binding energy and charge transfer than Pd-SWCNTs. The formation of C-Pd, N-Pd, C-Pt, and N-Pt bonds demonstrate that the metal atoms provide additional adsorptions sites for gases and open the possibility to use both materials as sensors for the detection of CO and NO.

6. Nanostructured oxides mixed with CNTs

Sensors made of metal oxides films have been used for a long time because of they provide high sensitivity for the detection of a wide variety of gases. However, their major drawback is their elevated operating temperatures. The development of metal-oxide NPs based films and nanocomposites has shown advantages like higher surface area and porosity, high catalytic activity, efficient charge transfer and adsorption capacity. However, it has been demonstrated that the improvements in gas detection at low temperature for CNTs/MO-based sensors is due to the introduction of CNTs in the nanocomposite.

Tin oxide (SnO2)/MWCNTS were synthesized using different ratios of tin dioxide precursor and plasma treated MWCNTs (Figure 6) [64]. The composites was tested for 2, 10, 20 ppm for CO and 50 100, 500, 1000 ppb of NO2 in dry air at both room temperature and 150 oC. Pure tin oxide films and pure plasma treated MWCNT were also tested for comparison purposes. Pure tin oxide films were unresponsive to all of the tested concentrations at the two different temperatures because both room temperature and 150 oC are too low when compared to the operation temperature for pure tin oxide-based sensors. On the other hand, pure plasma treated MWCNT responded to both gases at room temperature but not at 150 oC. As for the SnO2/MWCNTS composite, higher sensor response for both gases was achieved from samples prepared with an intermediate ratio of tin dioxide precursor and plasma treated MWCNTs (i. e. 20mL and 12mg, respectively), especially when operated at room temperature. Response time for 1 ppm of NO2 was 3minutesat 150 oC and 4 minutes at room temperature. Response time for 2 ppm of CO is stated to be 5 minutes but the temperature was not specified. SnO2/MWCNTS showed higher sensor response to NO2 than to CO, and was also sensitive to humidity changes.

Different composite synthesis temperature can affect the sensor performance. SnO2/SWCNTs composites were synthesized at different oxidizing temperatures (300-600 oC)for testing the effect of temperature in their morphology, structure and gas sensing properties in the detection of NO X [63]. The synthesized composites were exposed to 60 ppm of NO X at 200 oC and it was found that the ones synthesized at 400 oC showed higher response. From here, composites synthesized at 400 oC were exposed to 30 ppm NO X at different operating temperatures and it was determined that the optimum operation temperature was 200 oC. Concluding that the optimum oxidizing and operating temperatures were 200 oC and 400 oC, respectively, the samples were then exposed to different concentrations of NO X . Under the aforementioned conditions, the SnO2/SWCNTs composite showed improved performance for the detection of NO X when compared to thin films of SWCNTs or SnO2.


Figure 6.

Response of SnO2/MWCNTs to NO2 at (A) room temperature and (B) 150 oC. (From Leghrib et al. [64]. Copyright © 2010, with permission from Elsevier. )

Wongchoosuk, et al. were the first to report the preparation of MWCNT-doped tungsten oxide (WO3) thin films for H2 sensing application [65]. The thin films of MWCNT-doped WO3 and undoped WO3 (for comparison purposes) were prepared using the electron beam (e-beam) evaporation technique and exposed to 1000 ppm of H2 at different temperatures (200-400 oC). It was determined that 350 oC was the optimum operation temperature. Overall, MWCNT-doped WO3 thin films showed higher responses for H2 at any operating temperature when compared to the undoped WO3 thin film. To demonstrate selectivity, the response of the MWCNT-doped WO3 thin films was measured in presence of H2, ethanol (C2H5OH), methane (CH4), acetylene (C2H2) and ethylene (C2H4) at ppm level concentrations and operating temperature of 350 oC. It was concluded that the MWCNT-doped WO3 thin filmswere selective to H2 because they showed stronger response for H2, much weaker responses for C2H5OH, CH4, C2H2 and insensitivity ethylene (C2H4).

MWCNTs treated with nitric acid were used to fabricate MWCNTs-doped SnO2sensors for the detection of ethanol and liquid petroleum gases (LPG) [66]. Sensors were tested to 100-1000 ppm of ethanol and 1000-10, 000 ppm of LPG at different operation temperatures in the range of 10-360 oC. The detection of both chemicals was improved when the operating temperature was 350 oC or lower and it was determined that the optimum operating temperature is 320 oC. The MCNTs-doped SnO2 composite showed better selectivity for LGP than for ethanol and the calibration curve showed the sensors saturated at concentrations higher than 5000 ppm. The90% response and recovery time were 21s and 36s, respectively. When undoped SnO2 sensors were exposed to 250 ppm of ethanol and 2500 ppm of LPG, they showed higher sensitivity to ethanol than to LPG at operation temperature range of 190 - 360 oC. Considering the obtained results, the selectivity of the MCNTs-doped SnO2 composite for LGP can be attributed to the presence of MWCNTs but further studies are required.

Nanocomposite structures of cobalt oxide (Co3O4) and SWCNTs were prepared using a polymer assisted deposition (PAD) method [61]. For this, polyethyleneimine (PEI) was the polymer used to bind the cobalt ions from and adjust the viscosity of the solution during the deposition process in order to get a homogeneous distribution of the particles on the SWCNTs thin film. The Co3O4/SWCNTs composite sensor was tested for the detection of NOx in a concentration range of 20-100 ppm at room temperature. It showed proportional increases in response as function of concentration, poor recovery at room temperature and good recovery at 250 oC. Higher responses of the Co3O4/SWCNTs composite when compared to pristine CNTs are attributed to the high adsorption power of Co3O4 particles. The composite was also exposed to 4% of H2 in air, and showed enhanced responses than pure SWCNTs at room temperature and than Co3O4 films at both room temperature and 250 oC.

MO NPs (ZnO, SnO2, TiO2) and MWCNTs composites were simultaneously grown on silicon and silica on silicon substrates by catalytic pyrolysis method and used for gas sensing [60]. Current differential-voltage (∆I-V) curves were recorded for all the prepared composites, while to 100 ppm ethanol. TiO2/MWCNTs showed better sensitivity (defined as ∆I/I-V) when compared to pure MWNT film, ZnO/MWCNTs and SnO2/MWCNTs.

N-doped, B-doped and O-doped CNTs were used to prepare doped-CNTs/SnO2hybrids [67]. All doped-CNTs and doped-CNTs/SnO2hybrids were used to study the effect of functional groups on their gas sensing properties for 100, 200, 500, 1000ppb of NO2 at room temperature. The responses were as follows: B-doped hybrid> N-doped hybrid>O-doped hybrid. All doped-CNTs/SnO2hybrids responded better than N-doped and B-doped and O-doped CNTs. B-doped-CNTs/SnO2 hybrids showed an improvement in the response time when compared to bare CNTs and recovered its baseline, which was not achieved with B-doped CNTs. The high sensitivity and improved performance achieved with the B-doped and N-doped-CNTs/ SnO2 hybrids for low concentrations of NO2 at room temperature are attributed to two main factors: the interaction of the N2 gas with the n-SnO2/p-CNTs hetero-structure that affects the conduction of the CNTs and the addition of new functionalities (i. e. B and N atoms) to the CNTs surface that affects the electronic density of states and Fermi level and consequently, its conductivity.

A combination of ZnO layer with functionalized MWCNTs for the room temperature detection of NH3 has been reported by Tulliani and coworkers [62]. Samples of Pd-doped/COOH-MWCNTs, N-MWCNTs, and F-MWCNTs were deposited over a screen-printed ZnO layer. The materials were evaluated by measuring changes in resistance as the sensors were exposed to NH3 at room temperature, in a concentration range 0-75 ppm and different relative humidity levels. The sensor based on ZnO with Pd-doped/COOH-MWCNTs was the only one that showed sensitivity to humidity. When exposed to NH3, all sensors showed a decrease in electrical resistance but did not show better DL than other graphite-based sensors prepared under the same conditions.

7. Conclusion

Modification and functionalization of CNTs have shown to greatly improve the sensitivity and selectivity of CNTs-based sensors. For instance, great improvements for room temperature detection of different gases have been reported, especially when using metal oxide/SWCNTs composites. Another subject of high interest is the development of deposition methods and synthesis of Pd/CNTs for H2 detection at room temperature. Interestingly, there is an increase in the tendency of combining other materials with modified CNTs. For example, CNTs decorated with metal NPs embedded in a polymer matrix or CNTs doped or CNTs doped with heteroatoms and decorated with NPs or metal oxides are some composites that have been successfully used as gas sensing materials. But not only the characteristics of the CNTs have contributed to these improvements. In fact, the reported improvements are attributed to the combination of materials and the intrinsic characteristics of the composites. This trend of combining materials demonstrates that the there is broad range of possibilities for the design of new materials to meet the requirements of an ideal sensor by showing selectivity for different gases, sensitivity at low concentrations, fast response, and room temperature operation among others.


The authors would like to acknowledge the NASA-URC Center for Advanced Nanoscale Materials (CANM) Grant # NNX08BA48A and NNX10AQ17A, NASA GSRP fellowship under Grant # NNX09AM23H and NASA Ames Research Center-Nanosensor Group


1 - Niyogi S, Hamon MA, Hu H, Zhao B, Bhowmik P, Sen R, et al. Chemistry of single-walled carbon nanotubes. Acc Chem Res. 2002 Dec;35(12):1105-1113.
2 - Kong J, Franklin NR, Zhou CW, Chapline MG, Peng S, Cho KJ, et al. Nanotube molecular wires as chemical sensors. Science. 2000 Jan;287(5453):622-625.
3 - Ciraci S, Dag S, Yildirim T, Gülseren O, Senger RT. Functionalized Carbon Nanotubes And Device Applications. J Phys: Condens Matter. 2004;16(29):R901-R960.
4 - Chu H, Wei L, Cui R, Wang J, Li Y. Carbon nanotubes combined with inorganic nanomaterials: Preparations and applications. Coord Chem Rev. 2010;254(9–10):1117-1134.
5 - Liu S, Shen Q, Cao Y, Gan L, Wang Z, Steigerwald ML, et al. Chemical functionalization of single-walled carbon nanotube field-effect transistors as switches and sensors. Coord Chem Rev. 2010;254(9):1101-1116.
6 - Varghese OK, Kichambre PD, Gong D, Ong KG, Dickey EC, Grimes CA. Gas sensing characteristics of multi-wall carbon nanotubes. Sens Actuators, B. 2001;81(1):32-41.
7 - Wang Y, Yeow JTW. A Review of Carbon Nanotubes-Based Gas Sensors. Journal of Sensors. [electronic]. 2009;doi: 10.1155/2009/493904 (accessed 13 April 2012).
8 - Zhang T, Mubeen S, Myung NV, Deshusses MA. Recent progress in carbon nanotube-based gas sensors. Nanotechnology. 2008;doi: 332001 10.1088/0957-4484/19/33/332001 (accessed 13 April 2012).
9 - Zhang W-D, Zhang W-H. Carbon Nanotubes as Active Components for Gas Sensors. Journal of Sensors. 2009;doi: 10.1155/2009/160698 (accessed 13 April 2012).
10 - Di Francia G, Alfano B, La Ferrara V. Conductometric Gas Nanosensors. Journal of Sensors. 2009;doi:10.1155/2009/659275.
11 - Andzelm J, Govind N, Maiti A. Nanotube-based gas sensors - Role of structural defects. Chem Phys Lett. 2006 Apr;421 (1-3):58-62.
12 - Dai LM, Soundarrajan P, Kim T. Sensors and sensor arrays based on conjugated polymers and carbon nanotubes. Pure Appl Chem. 2002 Sep;74 (9):1753-1772.
13 - Goldoni A, Larciprete R, Petaccia L, Lizzit S. Single-wall carbon nanotube interaction with gases: Sample contaminants and environmental monitoring. JACS. [Article]. 2003 Sep;125 (37):11329-11333.
14 - Li J, Lu YJ, Ye Q, Cinke M, Han J, Meyyappan M. Carbon nanotube sensors for gas and organic vapor detection. Nano Lett. 2003 Jul;3 (7):929-933.
15 - Novak JP, Snow ES, Houser EJ, Park D, Stepnowski JL, McGill RA. Nerve agent detection using networks of single-walled carbon nanotubes. Appl Phys Lett. [Article]. 2003 Nov;83 (19):4026-4028.
16 - Valentini L, Armentano I, Kenny JM, Cantalini C, Lozzi L, Santucci S. Sensors for sub-ppm NO2 gas detection based on carbon nanotube thin films. Appl Phys Lett. 2003 Feb;82 (6):961-963.
17 - Lu YJ, Li J, Han J, Ng HT, Binder C, Partridge C, et al. Room temperature methane detection using palladium loaded single-walled carbon nanotube sensors. Chem Phys Lett. 2004 Jun;391 (4-6):344-348.
18 - Wang SG, Zhang Q, Yang DJ, Sellin PJ, Zhong GF. Multi-walled carbon nanotube-based gas sensors for NH3 detection. Diamond Relat Mater. 2004 Apr-Aug;13 (4-8):1327-1332.
19 - Lee CY, Strano MS. Understanding the Dynamics of Signal Transduction for Adsorption of Gases and Vapors on Carbon Nanotube Sensors. Langmuir. 2005 2005/05/01;21 (11):5192-5196.
20 - Penza M, Antolini F, Vittori-Antisari M. Carbon nanotubes-based surface acoustic waves oscillating sensor for vapour detection. Thin Solid Films. 2005 Jan;472 (1-2):246-252.
21 - Lu YJ, Partridge C, Meyyappan M, Li J. A carbon nanotube sensor array for sensitive gas discrimination using principal component analysis. J Electroanal Chem. 2006 Aug;593 (1-2):105-110.
22 - Robinson JA, Snow ES, Badescu SC, Reinecke TL, Perkins FK. Role of Defects in Single-Walled Carbon Nanotube Chemical Sensors. Nano Lett. 2006 2006/08/01;6 (8):1747-1751.
23 - Star A, Joshi V, Skarupo S, Thomas D, Gabriel J. Gas Sensor Array Based on Metal-Decorated Carbon Nanotubes. J Phys Chem B. 2006;110:21014 - 21020.
24 - Trojanowicz M. Analytical applications of carbon nanotubes: a review. TrAC, Trends Anal Chem. 2006 May;25 (5):480-489.
25 - Kuzmych O, Allen B, Star A. Carbon nanotube sensors for exhaled breath components. Nanotechnology. 2007; doi:10.1088/0957-4484/18/37/375502.
26 - Schlecht U, Balasubramanian K, Burghard M, Kern K. Electrochemically decorated carbon nanotubes for hydrogen sensing. Appl Surf Sci. 2007 Aug;253 (20):8394-8397.
27 - Valcarcel M, Cardenas S, Simonet BM. Role Of Carbon Nanotubes In Analytical Science. Anal Chem. 2007 Jul;79 (13):4788-4797.
28 - Endo M, Strano MS, Ajayan PM. Potential applications of carbon nanotubes. Carbon Nanotubes. 2008;111:13-61.
29 - Kauffman DR, Star A. Carbon nanotube gas and vapor sensors. Angewandte Chemie-International Edition. 2008;47 (35):6550-6570.
30 - Li C, Thostenson ET, Chou T-W. Sensors and actuators based on carbon nanotubes and their composites: A review. Compos Sci Technol. 2008;68 (6):1227-1249.
31 - Zanolli Z, Charlier JC. Defective carbon nanotubes for single-molecule sensing. Phys Rev B. 2009;doi:10.1103/PhysRevB.80.155447.
32 - Goldoni A, Petaccia L, Lizzit S, Larciprete R. Sensing gases with carbon nanotubes: a review of the actual situation. J Phys: Condens Matter. 2010; doi:10.1088/0953-8984/22/1/013001.
33 - Yoo K-P, Lim L-T, Min N-K, Lee MJ, Lee CJ, Park C-W. Novel resistive-type humidity sensor based on multiwall carbon nanotube/polyimide composite films. Sens Actuators, B. 2010;145 (1):120-125.
34 - Lu Y, Meyyappan M, Li J. Fabrication of carbon-nanotube-based sensor array and interference study. Journal of Materials Research. 2011;26 (26):2017-2023.
35 - Fam DWH, Palaniappan A, Tok AIY, Liedberg B, Moochhala SM. A review on technological aspects influencing commercialization of carbon nanotube sensors. Sens Actuators, B. 2011;157 (1):1-7.
36 - Lee S-H, Im JS, Kang SC, Bae T-S, In SJ, Jeong E, et al. An increase in gas sensitivity and recovery of an MWCNT-based gas sensor system in response to an electric field. Chem Phys Lett. 2010;497 (4):191-195.
37 - Cava CE, Salvatierra RV, Alves DCB, Ferlauto AS, Zarbin AJG, Roman LS. Self-assembled films of multi-wall carbon nanotubes used in gas sensors to increase the sensitivity limit for oxygen detection. Carbon. 2012;50 (5):1953-1958.
38 - Ndiaye AL, Varenne C, Bonnet P, Petit â, Spinelle L, Brunet Jrm, et al. Elaboration of single wall carbon nanotubes-based gas sensors: Evaluating the bundling effect on the sensor performance. Thin Solid Films. 2012;520 (13):4465-4469.
39 - Yao F, Duong DL, Lim SC, Yang SB, Hwang HR, Yu WJ, et al. Humidity-assisted selective reactivity between NO2 and SO2 gas on carbon nanotubes. J Mater Chem. 2011;21 (12):4502 - 4508.
40 - Chen G, Paronyan TM, Pigos EM, Harutyunyan AR. Enhanced gas sensing in pristine carbon nanotubes under continuous ultraviolet light illumination. Sci Rep. 2012;2:1-7.
41 - Battie Y, Ducloux O, Thobois P, Dorval N, Lauret JS, Attal-Trétout B, et al. Gas sensors based on thick films of semi-conducting single walled carbon nanotubes. Carbon. 2011;49 (11):3544-3552.
42 - Horrillo MC, Martí J, Matatagui D, Santos JP, Sayago I, Gutiérrez J, et al. Single-walled carbon nanotube microsensors for nerve agent simulant detection. Sens Actuators, B. 2011;157 (1):253-259.
43 - Wang F, Swager TM. Diverse Chemiresistors Based upon Covalently Modified Multiwalled Carbon Nanotubes. JACS. 2011 2011/07/27;133 (29):11181-11193.
44 - Shirsat MD, Sarkar T, Kakoullis J, Myung NV, Konnanath B, Spanias A, et al. Porphyrin-Functionalized Single-Walled Carbon Nanotube Chemiresistive Sensor Arrays for VOCs. The Journal of Physical Chemistry C. 2012 2012/02/09;116 (5):3845-3850.
45 - Penza M, Rossi R, Alvisi M, Signore MA, Serra E, Paolesse R, et al. Metalloporphyrins-modified carbon nanotubes networked films-based chemical sensors for enhanced gas sensitivity. Sens Actuators, B. 2010;144 (2):387-394.
46 - Tisch U, Aluf Y, Ionescu R, Nakhleh M, Bassal R, Axelrod N, et al. Detection of Asymptomatic Nigrostriatal Dopaminergic Lesion in Rats by Exhaled Air Analysis Using Carbon Nanotube Sensors. ACS Chemical Neuroscience. 2011;3 (3):161-166.
47 - Ionescu R, Broza Y, Shaltieli H, Sadeh D, Zilberman Y, Feng X, et al. Detection of Multiple Sclerosis from Exhaled Breath Using Bilayers of Polycyclic Aromatic Hydrocarbons and Single-Wall Carbon Nanotubes. ACS Chemical Neuroscience. 2011 2011/12/21;2 (12):687-693.
48 - Wei L, Shi D, Ye P, Dai Z, Chen H, Chen C, et al. Hole doping and surface functionalization of single-walled carbon nanotube chemiresistive sensors for ultrasensitive and highly selective organophosphor vapor detection. Nanotechnology. 2011;doi:10.1088/0957-4484/22/42/425501
49 - Wang Y, Yang Z, Hou Z, Xu D, Wei L, Kong ES-W, et al. Flexible gas sensors with assembled carbon nanotube thin films for DMMP vapor detection. Sens Actuators, B. 2010;150 (2):708-714.
50 - Slobodian P, Riha P, Lengalova A, Svoboda P, Saha P. Multi-wall carbon nanotube networks as potential resistive gas sensors for organic vapor detection. Carbon. 2011;49 (7):2499-2507.
51 - Cao CL, Hu CG, Fang L, Wang SX, Tian YS, Pan CY. Humidity Sensor Based on Multi-Walled Carbon Nanotube Thin Films. Journal of Nanomaterials. 2011;doi:10.1155/2011/707303.
52 - Liu C-K, Wu J-M, Shih HC. Application of plasma modified multi-wall carbon nanotubes to ethanol vapor detection. Sens Actuators, B. 2010;150 (2):641-648.
53 - Im JS, Kang SC, Bai BC, Bae T-S, In SJ, Jeong E, et al. Thermal fluorination effects on carbon nanotubes for preparation of a high-performance gas sensor. Carbon. 2011;49 (7):2235-2244.
54 - Xie H, Sheng C, Chen X, Wang X, Li Z, Zhou J. Multi-wall carbon nanotube gas sensors modified with amino-group to detect low concentration of formaldehyde. Sens Actuators, B. 2011;doi: 10.1016/j.snb.2011.12.112.
55 - Koós AA, Nicholls RJ, Dillon F, Kertész K, Biró LP, Crossley A, et al. Tailoring gas sensing properties of multi-walled carbon nanotubes by in situ modification with Si, P, and N. Carbon. 2012;50 (8):2816-2823.
56 - Battie Y, Ducloux O, Patout L, Thobois P, Loiseau A. Selectivity enhancement using mesoporous silica thin films for single walled carbon nanotube based vapour sensors. Sens Actuators, B. 2012;163 (1):121-127.
57 - Talla JA. First principles modeling of boron-doped carbon nanotube sensors. Physica B: Condensed Matter. 2012;407 (6):966-970.
58 - Talla JA. Ab initio simulations of doped single-walled carbon nanotube sensors. Chem Phys. 2012;392 (1):71-77.
59 - Hamadanian M, Khoshnevisan B, Fotooh FK, Tavangar Z. Computational study of super cell Al-substituted single-walled carbon nanotubes as CO sensor. Computational Materials Science. 2012;58:45-50.
60 - Liu H, Ma H, Zhou W, Liu W, Jie Z, Li X. Synthesis and gas sensing characteristic based on metal oxide modification multi wall carbon nanotube composites. Appl Surf Sci. 2012;258 (6):1991-1994.
61 - Li W, Jung H, Hoa ND, Kim D, Hong S-K, Kim H. Nanocomposite of cobalt oxide nanocrystals and single-walled carbon nanotubes for a gas sensor application. Sens Actuators, B. 2010;150 (1):160-166.
62 - Tulliani J-M, Cavalieri A, Musso S, Sardella E, Geobaldo F. Room temperature ammonia sensors based on zinc oxide and functionalized graphite and multi-walled carbon nanotubes. Sens Actuators, B. 2011;152 (2):144-154.
63 - Jang DM, Jung H, Hoa ND, Kim D, Hong S-K, Kim H. Tin Oxide-Carbon Nanotube Composite for NOX Sensing. Journal of Nanoscience and Nanotechnology. 2012;12 (2):1425-1428.
64 - Leghrib R, Pavelko R, Felten A, Vasiliev A, Cané C, Gracia I, et al. Gas sensors based on multiwall carbon nanotubes decorated with tin oxide nanoclusters. Sens Actuators, B. 2010;145 (1):411-416.
65 - Wongchoosuk C, Wisitsoraat A, Phokharatkul D, Tuantranont A, Kerdcharoen T. Multi-Walled Carbon Nanotube-Doped Tungsten Oxide Thin Films for Hydrogen Gas Sensing. Sensors. 2010;10 (8):7705-7715.
66 - Van Hieu N, Duc NAP, Trung T, Tuan MA, Chien ND. Gas-sensing properties of tin oxide doped with metal oxides and carbon nanotubes: A competitive sensor for ethanol and liquid petroleum gas. Sens Actuators, B. 2010;144 (2):450-456.
67 - Leghrib R, Felten A, Pireaux JJ, Llobet E. Gas sensors based on doped-CNT/SnO2 composites for NO2 detection at room temperature. Thin Solid Films. 2011;520 (3):966-970.
68 - Yun J, Im JS, Kim H-I, Lee Y-S. Effect of oxyfluorination on gas sensing behavior of polyaniline-coated multi-walled carbon nanotubes. Appl Surf Sci. 2012;258 (8):3462-3468.
69 - Mangu R, Rajaputra S, Singh VP. MWCNT–polymer composites as highly sensitive and selective room temperature gas sensors. Nanotechnology. 2011;doi:10.1088/0957-4484/22/21/215502.
70 - Sayago I, Fernández MJ, Fontecha JL, Horrillo MC, Vera C, Obieta I, et al. New sensitive layers for surface acoustic wave gas sensors based on polymer and carbon nanotube composites. Procedia Engineering. 2011;25 (0):256-259.
71 - Sayago I, Fernández MJ, Fontecha JL, Horrillo MC, Vera C, Obieta I, et al. New sensitive layers for surface acoustic wave gas sensors based on polymer and carbon nanotube composites. Sens Actuators, B. 2012;doi:10.1016/j.snb.2011.12.031.
72 - Sayago I, Fernández MJ, Fontecha JL, Horrillo MC, Vera C, Obieta I, et al. Surface acoustic wave gas sensors based on polyisobutylene and carbon nanotube composites. Sens Actuators, B. 2011;156 (1):1-5.
73 - Viespe C, Grigoriu C. Surface acoustic wave sensors with carbon nanotubes and SiO2/Si nanoparticles based nanocomposites for VOC detection. Sens Actuators, B. 2010;147 (1):43-47.
74 - Yun S, Kim J. Multi-walled carbon nanotubes-cellulose paper for a chemical vapor sensor. Sens Actuators, B. 2010;150 (1):308-313.
75 - Kumar B, Castro M, Feller JF. Poly (lactic acid)-multi-wall carbon nanotube conductive biopolymer nanocomposite vapour sensors. Sens Actuators, B. 2012;161 (1):621-628.
76 - Yuana CL, Chang CP, Song Y. Hazardous industrial gases identified using a novel polymer/MWNT composite resistance sensor array. Mater Sci Eng, B. 2011;176 (11):821-829.
77 - Li W, Hoa ND, Kim D. High-performance carbon nanotube hydrogen sensor. Sens Actuators, B. 2010;149 (1):184-188.
78 - Lvova L, Mastroianni M, Pomarico G, Santonico M, Pennazza G, Di Natale C, et al. Carbon nanotubes modified with porphyrin units for gaseous phase chemical sensing. Sens Actuators, B. 2011:doi:10.1016/j.snb.2011.1005.1031.
79 - Lu Y, Meyyappan M, Li J. Trace Detection of Hydrogen Peroxide Vapor Using a Carbon-Nanotube-Based Chemical Sensor. Small. 2011;7 (12):1714-1718.
80 - Lu Y, Meyyappan M, Li J. A carbon-nanotube-based sensor array for formaldehyde detection. Nanotechnology. 2011;doi:10.1088/0957-4484/22/5/055502.
81 - Ruiz A, Arbiol J, Cirera A, Cornet A, Morante JR. Surface activation by Pt-nanoclusters on titania for gas sensing applications. Materials Science and Engineering: C. 2002;19 (1-2):105-109.
82 - Ghasempour R, Mortazavi SZ, Iraji zad A, Rahimi F. Hydrogen sensing properties of multi-walled carbon nanotube films sputtered by Pd. Int J Hydrogen Energy. 2010;35 (9):4445-4449.
83 - Randeniya LK, Martin PJ, Bendavid A. Detection of hydrogen using multi-walled carbon-nanotube yarns coated with nanocrystalline Pd and Pd/Pt layered structures. Carbon. 2012;50 (5):1786-1792.
84 - Su P-G, Chuang Y-S. Flexible H2 sensors fabricated by layer-by-layer self-assembly thin film of multi-walled carbon nanotubes and modified in situ with Pd nanoparticles. Sens Actuators, B. 2010;145(1):521-526.
85 - Zilli D, Bonelli PR, Cukierman AL. Room temperature hydrogen gas sensor nanocomposite based on Pd-decorated multi-walled carbon nanotubes thin films. Sens Actuators, B. 2011;157 (1):169-176.
86 - Ju S, Lee JM, Jung Y, Lee E, Lee W, Kim S-J. Highly sensitive hydrogen gas sensors using single-walled carbon nanotubes grafted with Pd nanoparticles. Sens Actuators, B. 2010;146 (1):122-128.
87 - Rumiche F, Wang HH, Indacochea JE. Development of a fast-response/high-sensitivity double wall carbon nanotube nanostructured hydrogen sensor. Sens Actuators, B. 2012;163 (1):97-106.
88 - Sadek AZ, Bansal V, McCulloch DG, Spizzirri PG, Latham K, Lau DWM, et al. Facile, size-controlled deposition of highly dispersed gold nanoparticles on nitrogen carbon nanotubes for hydrogen sensing. Sens Actuators, B. 2011;160 (1):1034-1042.
89 - Penza M, Rossi R, Alvisi M, Serra E. Metal-modified and vertically aligned carbon nanotube sensors array for landfill gas monitoring applications. Nanotechnology. 2010;doi:10.1088/0957-4484/21/10/105501.
90 - Penza M, Rossi R, Alvisi M, Suriano D, Serra E. Pt-modified carbon nanotube networked layers for enhanced gas microsensors. Thin Solid Films. 2011;520 (3):959-965.
91 - Zhou X, Tian WQ, Wang X-L. Adsorption sensitivity of Pd-doped SWCNTs to small gas molecules. Sens Actuators, B. 2010;151 (1):56-64.
92 - Li K, Wang W, Cao D. Metal (Pd, Pt)-decorated carbon nanotubes for CO and NO sensing. Sens Actuators, B. 2011;In Press, Corrected Proof:doi: 10.1016/j.snb.2011.1006.1068.