Calculated adsorption energy, charge transfer and interacting distance.
The detection and analysis of SF6 decomposition components are of great significance in online condition assessment and fault diagnosis of GIS. Considering the shortcomings of general detection methods, carbon nanotubes (CNTs) gas sensor was studied to detect the SF6 decomposition components because of its advantages in large surface activity and abundant pore structure, et al. The large surface area has a strong adsorption and desorption capacity. In this chapter, SF6 decomposed gases, namely SO2F2, SOF2, SO2, H2S and CF4 are chosen as probe gases because they are the main by-products in the decomposition of SF6 under partial density (PD). First, the properties and preparation methods of CNTs are introduced to verify the advantages of CNTs for SF6 decomposition components detection. Then, both theoretical calculation and sensing experiment were adopted to study the microadsorption mechanism and macrogas-sensing properties. Based on the intrinsic CNTs, study for SF6 decomposition components adsorption, Pd, Ni, Al, Pt and Au metal doping CNTs and plasma-modified CNTs are discussed in order to enhance the gas sensing and selectivity of CNTs.
- SF6 decomposition components
- carbon nanotubes
- preparation method
- density functional theory
- metal doping
1. Introduction of carbon nanotubes
1.1. The properties of carbon nanotubes
1.1.1. Structure of carbon nanotubes
Carbon nanotubes (CNTs), which are also called the bucky tube, are a one-dimensional material with special structure. It is one allotrope of carbon, like the diamond, graphite and fullerene. In January 1991, a Japanese physicist Iijima first found CNTs produced during fabricating Carbon fiber using high-resolution transmission electron microscope . CNTs possess large aspect ratio because of its one-dimensional property. The electron wave function of CNTs exhibits periodic and translational invariance in radial and axial direction. A new strong atomic hybrid orbital is built by sp2 hybridization of carbon atoms, and CNTs skeleton of a hexagonal honeycomb is combined by σ bonds of carbon atoms. The isolated p electrons of Carbon atoms that did not participate in a hybrid together form conjugated π electron cloud across the entire CNTs. As shown in Figure 1, CNTs can be divided into single-wall carbon nanotubes (SWCNTs) and multi-wall carbon nanotubes (MWCNTs). Due to the unique molecular structure, CNTs have some specific properties in mechanics, electricity and heat.
1.1.2. Mechanical properties of carbon nanotubes
Carbon atoms in CNTs show sp2 hybridization, which have more s orbital compared with sp3 hybridization, and hence, the formed CNTs possess high modulus and strength. Its hardness is similar to that of diamond, while it also can be stretched due to its good flexibility. Like the reinforced fiber used in industry, the crucial factor that determines the strength of fiber is length to diameter ratio (at least 20:1). And the length to diameter ratio of CNTs has even reached 1000:1, making it an ideal fiber material with high strength, while the weight of CNTs is only 1/6–1/7 that of steel . Therefore, CNTs are also called “super fiber”. Besides, Krishnan et al. found that the Young’s modulus of SWCNTs along radial direction is up to 1 TPa measured by atomic force microscope .
1.1.3. The thermal properties of carbon nanotubes
CNTs show heat conduction anisotropy, showing high and low heat exchange in vertical and axial direction, respectively. Therefore, the high anisotropy of heat conduction material can be synthesized by controlling the orientation of the CNTs. The thermal conductivity of composites can be effectively improved by doping trace of CNTs.
1.1.4. The electrical properties of CNTs
The isolated p electrons of C atoms do not participate in a hybridization form a wide range of delocalized π bond due to the significant conjugative effect, making it possesses special electrical properties. As shown in Figure 2,
1.1.5. The electron emission property of carbon nanotubes
CNTs have a nanometer scale point, which is benefit for to the electrons emission. Hence, scientists predicted and verified that CNTs have an excellent field emission effect.
1.1.6. The adsorption characteristics
CNTs have large surface activity and abundant pore structure. And the large surface area of the gas phase chemical composition has a strong adsorption and desorption capacity.
1.2. Carbon nanotubes preparation methods
1.2.1. Arc discharge method
It is the first and most used method to prepare CNTs. The main process is: (a) keep a certain pressure of inert gas or hydrogen in vacuum vessel, (b) choose graphite (with catalyst: nickel, cobalt and iron) as electrode. The graphite is consumed by evaporation at anode during the arc discharge process, and CNTs are received by depositing at cathode. Ebbesn et al . successfully prepared gram order weight of CNTs under nitrogen gas condition, and then, this method is widely adopted. In 1994, Bethune introduced catalyst for arc reaction, reducing the reaction temperature and enhancing the productivity of CNTs. In 1997, Jounet et al. used catalysts for synthesizing single CNTs under helium condition. Sun Mingliang et al. studied the influence factors to CNTs prepared by DC arc discharge method: (a) inert gas pressure will affect the diameter and length of CNTs; (b) how much the adhesion of particles?; (c) oxygen and water vapor will lead to defects in CNTs, and it is unable to separate and purify after sintering together and (d) current and voltage will affect the yield and production rate of CNTs, but length to diameter ratio of graphite does not affect the generation of CNTs.
1.2.2. Catalytic cracking method
Catalytic cracking method, also known as chemical vapor deposition, prepares CNTs through cracking hydrocarbons or carbon oxides with the help of catalyst. The basic preparation process: (a) mixes the organic gases (such as acetylene and ethylene) with certain proportion of nitrogen gas in quartz tube. (b) CNTs grow on the surface of catalyst under certain temperature when the carbon source flow past and pyrolyze onto the surface of catalyst, and pushing forward the small catalyst particles . (c) The growth of CNTs ends till all of the catalyst particles were coated with graphite layer. The advantages of the method are: easy to control the reaction process, simple equipment, low raw material cost, easy to produce the product in large scale, and the high productivity. The disadvantages are: too much CNTs layers, poor graphitization and exist crystalline defects. These disadvantages have great adverse influence on the physical and chemical properties of CNTs.
1.2.3. Laser evaporation method
Laser evaporation method prepares CNTs by illuminating the graphite target that contains metal catalyst. Then, the vapor mixes with carbon source and deposits on the surface of substrate and the wall of reaction chamber. Smalley et al. received SWCNTs after adding a certain amount of catalyst to the electrode during preparing C60. After improving the method, Thess et al. successfully fabricated amount of SWCNTs. Under the condition of 1473 K, the graphite target with Ni/Co catalyst particles was irradiated by double pulse laser with 50 ns, receiving the high-quality SWCNTs bundles.
1.2.4. Low-temperature solid-state pyrolysis method
Low-temperature solid-state pyrolysis prepares CNTs through intermediate. First, the nanometer level silicon nitride (Si2C2N) ceramic intermediate was prepared. The nanoceramic intermediate is then placed in a boron nitride crucible, which is heated in a graphite resistance furnace to decompose it with nitrogen gas as the protective gas. After 1 h, the nanointermediate powder begins to pyrolyze, and the carbon atoms migrate to the surface. A high proportion of CNTs are obtained with amount of silicon nitride powder in the surface pyrolysis products. The advantage of the low-temperature solid-state pyrolysis method is the repeatable production, which is beneficial for large-scale CNTs production.
1.2.5. Polymer pyrolysis method
The method prepares CNTs by decomposition of hydrocarbons precursor (such as acetylene and benzene) at high temperature. Cho et al. prepared CNTs by heating the polymer obtained from citric acid and glycol after polyesterification under 400°C for 8 h. The CNTs were synthesized by using metal Ni as catalyst in the temperature ranged from 420 to 450°C and under H2 atmosphere. Under 900°C and Ar-H2 atmospheric conditions, Sen et al. obtained CNTs by pyrolyzing ferrocene, nickelocene and cobaltocene. These metal compounds not only provide carbon source after pyrolysis, but also provide the catalyst particles. The growth mechanism of the method is similar to the catalytic cracking method.
1.2.6. Ion (electron beam) radiation method
In a vacuum furnace, carbon is evaporated by ion or electron discharge and deposit on the condenser. Chernazatonskii et al. synthesized CNTs with diameter range from 10 to 20 nm and high alignment by evaporating the graphite coated on the surface of substrates. Lin X et al. got CNTs with diameter range from 10 to 15 nm by irradiating amorphous carbon with argon ion beam under high vacuum environment .
1.2.7. Flame synthesis method
Flame synthesis method utilizes the heat, produced by burning methane and a small amount of oxygen, and imports hydrocarbons and catalysts at temperature of 600–1300°C to synthesize CNTs. The CNTs prepared by this method have the disadvantages of low crystallinity and large amount of amorphous carbon. There is still no definite explanation for the growth mechanism of CNTs nanostructure by flame method. Richter et al. found SWCNTs that attached with a large amount of amorphous carbon from carbon black after burning the mixture of acetylene, oxygen and argon gases. Daschowdhury et al. found nanometer tubular CNTs by detecting carbon black after burning the mixture of benzene, acetylene, ethylene and oxygen gases.
1.2.8. Solar energy synthesis method
The CNTs are received from the condensation of high temperature (3000 K) mixture vapor of graphite and metal catalyst that heated by focusing the sunlight. This method is initially used for buckyballs production, then adopted for CNTs synthesis since 1996. Laplaze et al. synthesized the MWCNTs and SWCNTs use this method.
1.2.9. Electrolysis method
The preparation of CNTs by electrochemical method is a novel technique. This method adopts graphite electrode (electrolytic cell as anode), obtained carbon nanomaterials by electrolyzing molten alkali halide salts (such as LiCl) under a certain voltage and current with the protection of air or argon gases at about 600°C. The products include packaged or not packaged CNTs and carbon nanoparticles, and the form of carbon nanomaterials can be controlled by changing the process conditions of electrolysis. Andrei et al. found that CNTs can directly grow on the surface of n-type of (1 0 0) silicon electrode in solution of acetylene/ammonia. Hus et al. synthesized nanotubular and onion like CNTs under argon environment by using molten alkali metal halide as electrolyte and graphite as electrode. Huang Hui et al. successfully synthesized CNTs and carbon nanowires using LiCl and LiCl + SnCl2 as molten salt electrolyte.
1.2.10. Other methods
Stevens et al. got CNTs by using an exothermic reaction between caesium and nanoporous amorphous carbon in the low temperature of 50°C. Chemozatonskii et al. found the fullerene and CNTs at the microholes of Fe2Ni2C, Ni2Fe2C and Fe2Ni2Co2C alloy prepared by powder metallurgy method . Kyotani et al. first pyrolyze and deposit carbon on the wall of anodic alumina model (with nanometer trench) under 800°C. Then, hollow CNTs with open-end on both sides after removing the anodic alumina membrane by hydrofluoric acid can be obtained. Matveev et al synthesized CNTs using liquid nitrogen solution of acetylene at 233 K by electrochemical method. It is the lowest temperature ever reported to synthesize CNTs.
2. Modification CNTs
2.1. Simulation model build and computation method
This work chooses SWCNTs as a research object to present theoretical simulation for its adsorption of gas decomposition products of SF6 and then explores its adsorption characteristics and predicts the detectable gas products. Materials Studio (MS) software developed by Accelrys Company is employed in this research, the Dmol3 module of which is used for quantum mechanics stimulation. Generalized gradient approximation (GGA) approach, which can accurately describe the geometric and electronic structures of CNTs as well as the processes of molecular interaction, is adopted to deal with the interchange and correlation between electrons, and its specific form is Perdew-Burke-Ernzerhof (PBE) . The double-figure basis set (DNP) of polarization function is used in DFT (Density Functional Theory) calculation. In order to avoid the interactions between CNTs, a super grid 20 × 20 × 8.5 Å3 has been designed, working under periodic boundary conditions. The initial distance between SWCNT and gas decomposition products of SF6 is set as 0.16 nm. All atoms are calculated using full atomic potential, and the convergence value of self-consistent field is set as 10 × 10−5 eV/at . Ref.  has shown that accurate results can be achieved by taking two K points in the (8, 0) SWCNTs Brillouin zone. All calculations above are accomplished on Dmol3 module.
SWCNT, SF6 as well as its gas decomposition products including SF6, SO2F2, SOF2, SO2, H2S, CF4 and HF in the superlattices are optimized, respectively, to obtain the most stable structures before each calculation. Figure 3 presents the stabilized configuration of SWCNT gas molecules (SF6, SO2F2, SOF2, SO2, H2S, CF4 and HF) after geometrical optimization.
SF6 and decomposition gas molecules are made to approach the C atom marked on the SWCNT in any possible posture, which is optimized to form a stable molecule-SWCNT system, respectively. Then, stable configurations will be found after a non-restrictive optimization to the molecule-SWCNT systems, and their electron properties will be calculated .
To assess the ability to interact between SWCNT and gas molecules, the adsorption energy
The charge transfer
Besides, the highest occupied molecular orbital (HOMO) energy level and lowest unoccupied molecular orbital (LUMO) energy level were studied to evaluate the energy needed for electrons to cross the energy barrier based on the frontier molecular orbital analysis [10, 11]. After the adsorption, the energy gap of the adsorption structure can be calculated through the energy levels of
2.2. Gas-sensing properties of intrinsic SWCNTs to SOF2, SO2F2, SO2, H2S, HF, CF4 and SF6
2.2.1. Theoretical study: gas-sensing properties of intrinsic SWCNTs
22.214.171.124. The analysis of gas adsorption structure
We first studied the structure properties of pristine SWCNTs, Ni-SWCNTs, SO2, SOF2 and SO2F2. As an intrinsic structural beauty, SWCNTs consist of shells of sp2-hybridized (trivalent) carbon atoms  forming a hexagonal network that is itself arranged helically within a tubular motif shown in Figure 4a. The bond lengths of zigzag bond C─C2 (C1─C3) and axial bond C1─C4 were 1.44 and 1.41 Å, respectively. Figure 4 shows the most stable structures after gas molecules adsorb on the surface of intrinsic SWCNT. And the corresponding adsorption data are shown in Table 1.
It can be seen from Figure 4a, b and e and Table 1, the adsorption energy during the interaction of SF6, HF and CF4 with SWCNT is rather little, the adsorption energy of HF-SWCNT (−0.16 eV) is an order of magnitude lower than that of SF6-SWCNT (−2.17 eV), and then, the adsorption energy of CF4-SWCNT (−0.02 eV) is two orders of magnitude lower than that of SF6-SWCNT; however, in terms of charge transfer, the number of charge transfer (0.038 au) between SWCNT and HF is an order of magnitude higher than that (0.005 au) between SWCNT and SF6, while the number (0.003 au) between SWCNT and CF4 is still lower than that, but in fact, the interacting distance is similar in the interaction of HF and CF4 with SWCNT. As is shown above that SWCNT is insensitive to HF and CF4 .
From Figure 4c, d and f and Table 1 , it is clear that the adsorption energy during the interaction of H2S, SO2 and SOF2 with SWCNT is almost in the same level; the number of charge transfer between SWCNT and H2S (0.008 au) is a bit higher than that between SWCNT and SF6 (0.005 au); however, they are in the same order of magnitude, while the number of charge transfer between SWCNT and SO2, SOF2 is an order of magnitude higher than that between SWCNT and SF6. But the interacting distance is similar in the interaction of SO2, SOF2, SF6 with SWCNT. It means the sensitivity of SWCNT to H2S, SO2 and SOF2 is the same as that to SF6, so there is cross-sensitivity between them. Under the background of the high concentration of SF6, SWCNT as a gas sensor is unable to accurately detect H2S, SO2 and SOF2.
Figure 5 presents the most stable configurations of SO2F2-SWCNT. Figure 5a presents the chart whose chemical bond is not displayed; Figure 5b gives the chart whose chemical bond is displayed by MS. From Figure 5b, it is seen that the S atom in SO2F2 has formed the bond with the C atom marked in SWCNT, and the F atom has formed the bond with adjacent C atom yet, which means that the chemisorption between SWCNT and SO2F2 occurs. It can be inferred based on the data above that the adsorption energy of SO2F2-SWCNT is lower 0.98 eV than that of SF6-SWCNT, but they are in the same order of magnitude, which shows that there exist differences between them. However, the number of charge transfer (0.403 au) between SWCNT and SO2F2 is 80 times higher than that (0.005 au) between SWCNT and SF6, which shows that the conductivity of SWCNT has changed a lot after adsorbing SO2F2. The interacting distance during the interaction of SO2F2 with SWCNT is obviously less than that of other molecules. Therefore, it can be concluded that SWCNT is the most sensitive to SO2F2 in all the gas decomposition products of SF6.
126.96.36.199. The analysis of the density of states
From Figure 6, it is clear that the density of states curves of SWCNT almost coincides after adsorbing HF, H2S and CF4 , which reveals that the electronic structures and conductive properties of SWCNT are basically unchanged, so SWCNT is not sensitive to HF, H2S, and CF4. However, the density of states curves shifts to the right of Fermi level after SOF2 and SO2 are absorbed, which indicates that the electronic structures are changed. There is a short overlap of DOSs between SWCNT and SO2-SWCNT near Femi level, so the conductive properties change a little. But the DOSs peak of SOF2-SWCNT is lower than that of SWCNT in the Fermi energy level, which means that the number of quantum states occupied by electrons in the Fermi energy level has reduced when SOF2 molecules adsorbed on SWCNT, causing SWCNT’s conductivity decreased. Finally, it can be concluded that the sensitivity of SWCNT to SO2 is similar to SOF2 .
From the Figure 7, it can be derived that DOSs has changed a lot after absorbing SF6, SO2F2 in and near the Fermi level. DOSs curve of SO2F2-SWCNT is higher than SWCNT’s, while DOSs curve of SF6-SWCNT is lower than SWCNT’s. The number of quantum states occupied by electrons near the Fermi energy level has increased after SO2F2 adsorbed by SWCNT, the properties of SWCNT becoming more active and conductivity being enhanced, on the contrary, the properties of SWCNT become less active after absorbing SF6. Based on the analysis above, SWCNT is the most sensitive to SO2F2.
Band structures of SWCNT, SF6-SWCNT and SO2F2-SWCNT are given in Figure 8a–c, from which we can see that the energy gap (Eg1 of SWCNT is about 0.022 ha (0.60 eV), SF6-SWCNT (Eg2 is about 0.022 ha (0.60 eV) and SO2F2-SWCNT (Eg3) is about 0.015 ha (0.40 eV), which reveals that the conductivity is unchanged after absorbing SF6, but the conductivity is increased after absorbing SO2F2. Thus, it can be predicted that SWCNT can serve as gas sensors to detect SO2F2, one of the decomposing gas products of SF6, in partial density (PD).
2.2.2. Experimental study: gas-sensing properties of intrinsic SWCNTs
188.8.131.52. Preparation of plasma-modified intrinsic SWCNTs
MWCNTs (tube diameter, 20 to 30 nm; length, 10 to 30 μm; purity, >95%) were grown by chemical vapor deposition (CVD) in black powder and purchased from the Chengdu Institute of Organic Chemistry Chengdu, China. CNTs are one-dimensional (1D) nanomaterials. Hence, appropriate surface processing parameters should be selected. Under strong plasma treatments, high power and long treatment time can destroy the tubular structure and carbonization of CNTs [13, 14]. In this study, a DBD plasma generator was used to modify MWCNTs. Figure 9 shows the schematic for the test device. Low-temperature plasma experimental power (CTP-2000K) used in this experiment was produced from Nanjing Rongman Electronics Co., Ltd., China. The input voltage of the experimental power is controlled by a voltage regulator. Adjust the voltage to 30 V, which can be reading from the Voltmeter (Power input) in the power device. Adjust output frequency knob in the experimental power until frequency is around 10 kHz. Then, we can get an optimum DBD discharge. Read the input current of 1.96 A from Ammeter in the power device. Using oscilloscope to obtain the output voltage and current waves, and displayed in Figure 9. We should point out that there is an attenuator in this experimental power, and the attenuation coefficient is 1000. So the output peak-to-peak voltage is 39.3 kV. The discharge power in DBD plasma reactor can be calculated by Lissajou curve. However, due to the poor laboratory conditions, we do not have enough oscilloscope attenuation probes to protect oscilloscope from breakdown. So other method should be explored, and we try to get in touch with the equipments manufacturers. According to the experience of the manufacturer’s data, the plasma treatment power is approximately 0.8 times of the input power at the same experimental conditions. Therefore, we can calculate the discharge power which is 47 W.
Figure 10 reveals that the shape of the reactor is similar to a Petri dish. The reactor electrodes formed a parallel-plate structure and were made of 2-mm thick quartz glass. The upper and bottom electrodes were 8 mm apart. The bottom quartz glass electrode adhered to the reaction kettle, whereas the upper electrode is removable. In the modified experiment, an adequate amount of MWCNTs was placed in a reaction kettle and sealed with silicone to ensure gas tightness. Air was released from the reactor to induce a vacuum state. CF4 flow rate was controlled at 150 sccm. The parameters of the experimental power were adjusted, and MWCNTs were, respectively, treated for 0.5, 1, 2, 5, 8, 10 and 12 min. The upper quartz glass was removed, and modified MWCNTs were obtained after the treatment.
184.108.40.206. Preparation of plasma-modified MWCNTs-based sensors
MWNT sensors were made of printed circuit board, and the substrate material is epoxy resin. Cu interdigital electrodes were etched in the substrate. The width and spacing of the electrodes are both 0.2 mm. First, MWCNTs were placed into a beaker containing the appropriate ethanol solution. The beaker was placed in an ultrasonic bath for 1 h. Then, the sensor substrate was repeatedly cleaned with deionized water to remove impurities on the electrode surface. Next, the mixed solution was dropped on the substrate surface. Finally, the MWNT-coated substrates were baked in an oven at 80°C for a specific time. This process was repeated several times until uniform MWCNTs films were deposited on the surface. Seven pristine and treated MWCNTs with different modification times were used to fabricate the gas sensors.
220.127.116.11. Characterization of plasma-modified MWCNTs
FTIR spectra are highly useful tools to analyze the characteristics of CNTs. Figure 11 shows the FTIR spectra of pristine MWCNTs and those generated by CF4 plasma etching for 1, 5 and 10 min with a Nicolet 5DXCFT-IR spectrometer.
Diverse functional groups and types of bonding were observed in the FTIR spectra of MWCNTs (Figure 11). The absorption peaks at 3445 cm−1 corresponded to the ─OH groups in pristine and treated nanotubes. The absorption peaks at 1036 and 1151 cm−1 were ascribed to the respective C─F and symmetric ─CF2 stretching vibrations because of the CF4 plasma treatment.
The surface morphologies of the pristine and plasma-treated MWCNTs were analyzed using Zeiss Auriga focused ion beam and double-beam emission scanning electron microscopy (SEM). The SEM images of pristine MWCNTs (Figure 12a) indicated the presence of several small particles, which included amorphous carbons and residual catalysts during preparation. Figure 12b and c shows the SEM images of CF4 plasma treated for 10 min. The impurities and dopant on the nanotubes surfaces were removed, and MWCNTs became shorter. Plasma treatment retained the nanotubes structures.
18.104.22.168. The analysis of the gas-sensing properties
We used eight kinds of MWCNTs-based gas sensors (pristine MWCNTs and MWCNTs modified by plasma for different time) to detect H2S and SO2 whose concentration is both 50 ppm. The gas response curves are shown in Figure 13. It can be seen from Figure 13a and b that the sensitivity of pristine MWCNTs and those modified by CF4 plasma for 0.5, 1 and 2 min to H2S are 3, 3.2, 3.4 and 3.5%, respectively, and to SO2 are 2.3, 2.4, 2.6 and 2.7%. Obviously, after modification, the gas sensitivities of MWCNTs are not markedly enhanced. Under small discharge power, these phenomena may have been caused by the insufficient treatment time and poorly surface modification. Therefore, if the discharge power remains unchanged, in order to achieve a better surface modification, plasma treatment time should be extended.
In consequence, Figure 13c and d shows the response curves of pristine MWCNTs and these treated for 5, 8, 10 and 12 min to H2S and SO2. We can see that when the treatment time is less than 10 min, the sensitivities of MWCNTs sensors increased with increasing of treatment time. Meanwhile, the MWCNTs modified by CF4 plasma for 10 min exhibited the best sensitivity both to H2S and SO2. However, the sensitivities decreased when the treatment time is over 10 min. Possible reasons may be that after longer treatment time, the structure of the nanotubes was destroyed, and nanotubes were partly carbonized  under the bombardment of energetic particles in prolonged plasma treatments, which result in a reduce of active adsorption sites on MWCNTs surface for gas molecules. Hence, the gas-sensing properties of the MWCNTs were affected.
Figure 13 reveals that the response time of CF4 plasma-modified MWCNTs sensors to H2S and SO2 was shorter. For treatment times ranging from 0 to 10 min, the response time decreased with increasing treatment time. Besides, the shortest response times to H2S and SO2 are 70 and 150 s, respectively.
Responses of MWCNTs-based sensors to H2S and SO2 at different concentrations are studied in this work. MWNT sensors modified by CF4 plasma for 10 min (Section 3.3) were selected to detect H2S and SO2 at 10, 25, 50 and 100 ppm because these sensors yielded the best sensitivities. Figure 14a and b indicates that the sensitivity of the sensors increases with the gas concentration.
Figure 15 shows that the gas concentration and sensor sensitivity were linearly correlated for H2S and SO2 concentrations of 10–100 ppm with correlation coefficients (
22.214.171.124. Desorption and repeatability of MWCNTs-based sensors
To analyze the desorption properties of modified MWCNTs gas sensors, these modified by CF4 plasma for 10 min were chosen to test the recovery curve, as shown in Figure 16. The experiment steps are as follows. Firstly, the chamber was pumped into vacuum and standing for a period of time. After resistance of the sensor remains unchanged, in the second minute 50 ppm, H2S was introduced into the chamber, and the resistance showed a quick decrease. Few minutes later, the resistance of sensor remains stable. Currently, H2S gas molecules reach adsorption equilibrium at the surface of MWCNTs. In the fifth minute, pure N2 was injected into the gas chamber, and the sensor resistance can generally recover near the initial value. There still have a small amount of residual gas accumulates on the surface of the sensor which affect the sensitivity. In order to obtain a completely desorption, placed the sensor under UV irradiation. By irradiating with UV light, the residual gas absorbs energy, which enables it to “escape” from the “trapped” state where almost no residual gas remains on the surface of the tested sensor. After N2 and UV treatments, the sensor resistance was gradually restored to its initial value. The recovery time was about 25 min, which was less than that of the pristine MWCNTs sensor to H2S (40 min; data not shown).
The MWCNTs sensor modified by plasma for 10 min that was most sensitive to SO2 was selected to illustrate the repeatability process (Figure 17). The resistance-change trends remained similar, and the maximum resistance-change rate remained the same and stable. Hence, the gas sensor could be repeatedly used with good response and stability. However, the recovery time was approximately 35 min and was not greatly enhanced in contrast to that of pristine MWNT-based sensors.
126.96.36.199. Gas-sensing mechanism
The CF4 plasma-modified MWCNTs sensors exhibited high sensitivities to H2S and SO2 because of the following reasons: (1) The accelerated electrons, ions and free radicals cleaned the MWNT surface by etching some amorphous carbon and catalyst particles during plasma treatment; (2) the bombardment of energetic particles destroyed some of the nanotubes and increased the defects on their surfaces, which generated effective adsorption sites for gas molecules; and (3) CF4, a fluorinated gas , was ionized to generate fluoride ions in DBD and react with carbon atoms on the MWCNTs surface to yield C─F bonds  without destroying the tubular structure. Given the strong polarity and reactivity of F atoms, fluorinated MWCNTs exhibited strong adsorption capacities and high gas-sensing properties.
The response and recovery time of plasma-modified MWNT sensors to H2S were remarkably reduced, but only the response time to SO2 decreased, and recovery time was not reduced (Section 3.5). Theoretically, H2S molecules were physically adsorbed on the surface of MWCNTs through van der Waals interaction. However, some hydroxyls existed on the surfaces of the nanotubes during growth by CVD. F atoms were introduced onto the MWCNTs surface after fluorination. C─F bonds possessed high polarity because of the strong electro negativity of the F atom, during which ─F was essential. Stable hydrogen bonds (C─F…H─S) were formed between H atoms in H2S molecules and F atoms when H2S molecules were adsorbed on the surface of modified MWCNTs. Subsequently, the van der Waals forces were replaced, and the adsorption of H2S molecules was accelerated to reduce the response time (Figure 18a). In addition, O atoms in the hydroxyl groups in MWCNTs surfaces exhibited small atomic radii and high electro negativities. Hydrogen bonds (C─O…H─S) were formed between O atoms in hydroxyl and H atoms in H2S molecules (Figure 18a). The recovery time of plasma-based MWCNTs sensors to H2S decreased possibly because of the effect of UV irradiation that the H─F bond is easier to disintegrate. For SO2, only O atoms in the SO2 molecules and H atoms of hydroxyl were combined to form hydrogen bonds [O─H…O─S; Figure 18b]. F atoms on the surfaces of modified MWNT increased the number of effective adsorption sites for gas molecules, accelerated the adsorption and reduced the response time. However, the recovery time remained invariant.
2.2.3. Summary: gas adsorption on intrinsic SWCNT
In the theoretical study aspect, the adsorption between SWCNT and SO2F2 was chemisorption because new covalent bonds were formed. The number of charge transfer between SWCNT and SO2F2 was 80 times higher than that of between SWCNT and SF6, and also higher than that of other gas decomposition products, which show that the adsorption is the strongest. The calculated DOSs indicated that the SO2F2 gas molecules adsorbed on SWCNT had changed the electronic structures of SWCNT, chemical properties of SWCNT becoming more active. In fact, the conductivity of SWCNT was also enhanced because the energy gap of SWCNT had decreased from 0.022 ha (0.60 eV) to 0.015 ha (0.40 eV) when the SO2F2 gas molecules were adsorbed. However, HF, H2S and CF4 molecules adsorbed on SWCNT had little effect on the electronic structures of SWCNT, so SWCNT’s properties kept unchanged. Due to the cross-sensitivity of SWCNT to SF6, SO2 and SOF2 molecules, SWCNT cannot detect the SO2 and SOF2, respectively. Thus, based on the analysis above, SWCNT can be prepared a gas sensor to detect SO2F2 gas among the gas decomposition products of SF6 in PD.
In the experimental study aspect, MWCNTs grown by the CVD method are initially modified by atmospheric pressure DBD air plasma and are used as gas-sensitive materials. Then, the gas sensitivity of the unmodified and modified MWCNTs to 50 ppm H2S and 50 ppm SO2 is tested, respectively. The results show that the sensitivity of modified MWCNTs to H2S is enhanced 2.75 times, and the response time to H2S greatly reduced . However, the sensitivity of modified MWCNTs to SO2 exhibits the opposite effect. The MWCNTs are almost no longer sensitive to SO2. Thus, the MWCNTs modified by atmospheric pressure DBD air plasma presented good selectivity to H2S and have great potential value in the detection of this gas .
2.3. Gas-sensing properties of Pd-SWCNTs to SOF2, SO2F2, SO2, H2S, HF, CF4 and SF6
2.3.1. Structural parameters of intrinsic Pd-SWCNTs
The geometric structure of the SWCNTs is dramatically distorted after substitution as shown in Figure 19. The impurity of the Pd atom induces the deformation of the six-membered ring near the doping site to relieve stress, which results in the carbon site substituted by the Pd heteroatom that evidently protrudes out of the tube wall because the radii of the Pd atom are larger than other carbon atoms [17, 18].
2.3.2. The analysis of gas adsorption structure
The SO2, H2S, SOF2, SO2F2 and CF4 gas molecules were made to approach the Pd atom marked on the SWCNTs at any possible posture to find the most stable adsorption system (see Figure 20). The adsorption energy
Pd acts as the adsorption site in the process of SO2 adsorption. When one SO2 molecule approaches the Pd atom and the adsorption structure is optimized to find the steady state (Figure 20a1), the two oxygen atoms labeled O1 and O2 are seen close to the Pd atom, whereas the S atom is seen away from the Pd atom, indicating that the Pd and O atoms form a coordinate bond, and the interaction between the Pd and S atoms is weak. The interatomic distance S─O1 changes from 1.480 to 1.565 Å, and the Pd-O1 distance is 2.281 Å in the reaction process, indicating that SO2 adsorbed on the surface results in the elongation of the S─O bond. The result is agreement with our previous study , where the interaction distance between the Pd atom and the SO2 in our present Pd-doped (8, 0) SWCNTs is generally slightly smaller than that of Pd-doped (5, 5) SWCNTs . The long molecule surface distance 2.281 Å and low banding energy −0.798 eV suggest some kind of physisorption. Upon the adsorption of the second SO2 molecule on Pd-SWCNTs (Figure 20a2), the two molecules become simultaneously close to the Pd atom through the oxygen atom O1ʹ and O2ʹ. The adsorption distance of Pd-O1ʹ and Pd-O2ʹ is 2.231 and 2.236 Å, respectively, which shows no distinct difference to that of single SO2 adsorption, whereas the interatomic distance of SO2 becomes slightly elongated compared with the individual molecule causing increased bonding strength between the Pd atom, O1ʹ, and O2ʹ.
The optimized structures of H2S adsorbed on Pd-SWCNTs are shown in Figure 20b1 andb2. The interaction between H atoms of H2S and Pd is too weak, and thus, adsorption of H2S through S atom is an appropriate adsorption conformation course for the multiple valence states of the S atom. Upon single molecule adsorption, a quasi-tetrahedron geometry around the Pd center with H2S forms in one of the apical positions upon adsorption of H2S. The Pd-S long distance 2.570 Å and the low banding energy −0.802 eV are received in the process of adsorption, which suggests that H2S undergoes moderate physisorption. After the second H2S approached the Pd-SWCNTs, both H2S molecules were situated around the Pd atom in a similar geometrical morphology. The results showed that Pd-SWCNTs had similar adsorption ability with both of the H2S molecules. The total adsorption energy of the two H2S molecules has reached −1.361 eV with Pd-S1ʹ and Pd-S2ʹ distance of 2.689 and 2.588 Å, respectively. The adsorption energy has been much enhanced than our previous studied gold doped (8, 0) SWCNT . The H2S molecules act as electron donor, and the charge transfer QT is 0.481 e. The large adsorption energy and considerable charge transfer made the Pd-SWCNTs a possible sensor material to detect H2S. Star et al. reported that Pd-Decorated CNTs show good response to 50 ppm H2S using the experimental method .
The adsorption of SOF2 on the surface of Pd-doped (8, 0) SWCNTs is more stable from the F atom toward the Pd site, as shown in Figure 20c1 and c2. The calculated binding energy for the SOF2 interacted across the Pd atom of (8, 0) SWCNTs is −0.846 eV, and the adsorption distance between the F1 atom of molecule and the Pd atom of tubes is 2.003 Å, whereas the distance between F1-S bond increased to 2.778 Å. The large binding energy and structure change shown by the SOF2 molecule presents a strong chemical interaction with the Pd-doped SWCNTs . The Mulliken population analysis showed that the SOF2 adsorption on Pd-doped (8, 0) SWCNTs leads to 0.572 electron transfer from the tubes to the SOF2 molecule. Therefore, SOF2 functions as an electron acceptor, whereas the nanotube functions as an electron donor. From Figure 20c2, we found that the adsorption distance between the second SOF2 and the Pd-SWCNTs was 4.649 Å. Therefore, the adsorption is obviously weaker than the first adsorbed Pd-SWCNTs. The increased adsorption energy induced by the second SOF2 is only −0.178 eV, which has also confirmed the weak interaction between the second SOF2 molecule and Pd-SWCNTs. To some extent, the result can be attributed to the strong repulsive force between the SOF2 molecules. Meanwhile, the charge transfer
In the adsorption of SO2F2 (Figure 20d1 and d2), although the adsorption energy value of single SO2F2 molecule is in the same order of magnitude as SO2 and SOF2, the adsorption energy of SO2F2 (−1.627 eV) is still almost twice over SO2 (−0.798 eV), SOF2 (−0.846 eV), and even reached 20 times more that the value of CF4 (−0.086 eV). The interatomic distance S-F1 increased from 1.611 to 3.124 Å with an S-Pd distance of 2.004 Å. Therefore, we concluded that Pd doping makes the SWCNTs preferable for SO2F2 chemisorption. The adsorption of two SO2F2 is similar to SOF2, which is the first SO2F2 near the Pd atom with a binding distance of −2.025 Å. The second molecule from the Pd atom with a distance of 4.183 Å creates the repulsive force between the SO2F2 molecules. The total adsorption energy is Pd atom 1.735 eV, and the charge transfer is −0.973 electron, which are almost the same with the values of single SO2F2 adsorption.
The adsorption of CF4 (Figure 20e1 and e2) is only −0.046 eV because of weak van der Waals interaction between two species, and nearly no charge transfer was present . The energy is the least one among all gas molecules adsorption. The interacting distance from Pd atom to the atom F1 is 3.507 Å. Upon the two molecules’ adsorption, the Pd-F1ʹ and Pd-F2ʹ are 3.243 and 3.287 Å. The conductivity of Pd-SWCNTs before and after adsorption may change little because of the large interaction distance.
2.3.3. The analysis of the density of states and Frontier molecular orbital
Large charge transfer affects the density of states (DOS) near the Fermi level and brings about significant differences in frontier molecular orbitals . To further elucidate the electronic properties of the Pd-SWCNTs and molecule-Pd-SWCNTs, total electronic density of states (TDOS) and local DOS of a group (Pd or molecule) (LDOS) are depicted to investigate the influence of gas adsorption  in Figure 21. To further study the electronic structure of the Pd-SWCNTs and molecule-Pd-SWCNTs near the Fermi level, the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) in the molecule adsorption on the Pd-doped SWCNTs are listed in Table 3. The diagrams of HOMO and LUMO are depicted in Figure 22.
|System||EHOMO (eV)||ELUMO (eV)||EL-H (eV)|
From Figure 21, we found that the LDOS of Pd atom has little contribution to each TDOS and that the changes of TDOS are mainly from the adsorbed molecules. As plotted in Figure 21a1, the DOS of Pd-doped SWCNTs is continuous at Fermi level, which suggests that Pd-doped SWCNTs is a conductor. Upon adsorption of SO2 molecule in Figure 21b1 and b2, the TDOS near Fermi level evidently increased, and the DOS at Fermi level was enhanced when the adsorbed SO2 molecule increased. In Figure 22b1, the HOMO of the SO2-Pd-SWCNTs was mainly constituted by the Pd and SO2, and the p orbital of S and O atoms interacted with the d orbitals of the Pt atom. The LUMO is localized on the SWCNTs, as seen in Figure 22b2. After the other SO2 molecule approached the Pd atom in Figure 22b3 and b4, the LUMO significantly transferred to the SO2 molecules. The HOMO-LUMO energy gap of the SO2-Pd-SWCNTs is only 0.066 eV, which is 0.279 eV smaller than that of bare Pd-SWCNTs. Although the HOMO-LUMO energy gap of the 2SO2-Pd-SWCNTs is slightly bigger than single molecule adsorption, it was still 0.229 eV smaller than individual Pd-SWCNTs. The decrease of HOMO-LUMO energy gap associated with the significantly enhanced in the TDOS near the Fermi level suggests that the adsorption of SO2 largely increases conductance. According to the results reported by Camilli G et al. , using armchair Pd SWCNTs resulted in the reduction in the HOMO-LUMO energy gap of single and dual H2S molecule adsorption by 0.17 and 0.16 eV, respectively. Meanwhile, the TDOS change introduced by the second SO2 molecule showed no significant difference. Pd-doped zigzag SWCNTs show preferable sensitivity to SO2.
According to the H2S molecules adsorbed on Pd-SWCNTs, the TDOS at Fermi level showed no change whether single or dual H2S adsorption in Figure 21c1 and c2 occurred. In Figure 22c1–c4, almost the entire HOMO and LUMO were on Pd-SWCNTs. The HOMO-LUMO energy gap of H2S-Pd-SWCNTs and 2H2S-Pd-SWCNTs is 0.322 and 0.267 eV, respectively, which is slightly decreased compared with the bare Pd-SWCNTs. The results are consistent with the adsorption configurations. Given that the H atoms have formed a covalent bond with the S atom, the H2S molecules can only interact with Pd-SWCNTs by S atoms. Although S atom forms the interaction with Pd atom, the primary S-H bond makes it hard to build strong interaction with the Pd-SWCNTs. The same result is seen in Pt-doped SWCNTs . The small change at Fermi level in the H2S adsorption process indicates little change in conductivity, which limits the performance of Pd-SWCNTs to detect the H2S gas in SF6 decomposition components.
Upon SOF2 adsorption, as seen in Figure 22d1 and d2, the p orbital of S atom and d orbital of Pt atom form a δ bonding orbital in the HOMO. In the LUMO, the p orbital of S atom in SOF2 overlaps with the d orbital of Pt atom. The HOMO and LUMO energies of SOF2-Pd-SWCNTs are slightly reduced with respect to those of bare Pd-SWCNTs. The HOMO-LUMO energy gap diminished to 0.179 eV. The decrease of the HOMO-LUMO energy gap would result in increased electron transfer to gas molecule. As we have already mentioned, the second SOF2 molecule is far from the Pd atom. Therefore, the LDOS of the second SOF2 brings little contribution to TDOS of adsorption system (Figure 21d1 and d2). The HOMO and LUMO of 2SOF2-Pd-SWCNTs in Figure 22d3 and d4 have also confirmed the analysis results, neither the HOMO nor the LUMO is located on the second SOF2 molecule. Therefore, conductivity does not increase with the rise of SOF2 molecule number adsorbed on Pd-SWCNTs.
From the orbital of single SO2F2 adsorbed on Pd-SWCNTs in Figure 22e1, we can see a weak bond between the molecule and the Pd-SWCNTs. The HOMO-LUMO energy gap is 0.415 eV, which increased with the energy gap in other molecule adsorption. It greatly reduces the electron transition probability between HOMO and LUMO. Similar to the second SOF2 adsorption, the adsorption system keeps its original characteristics after the second SO2F2 adsorbed on Pd-SWCNTs in Figure 22e2. In addition, the TDOS of SO2F2 adsorbed Pd-SWCNTs at the Fermi level is weaker than individual Pd-SWCNTs. Considering the molecule frontier orbital and TDOS, we assumed that SO2F2 adsorption will result in the decrease of conductance.
Upon the adsorption of CF4, the LDOS introduced by CF4 mainly under the Fermi level was not significant (Figure 21f1 and f2). Furthermore, the HOMO and LOMO were almost identical to that of Pd-SWCNTs, as shown in Figure 22f1–f4. Considering the frontier orbital and TDOS, we predicted that the Pd-SWCNTs are insensitive to CF4 detection.
2.3.4. Summary: gas adsorption on Pd-SWCNTs
Adsorption of SF6 decomposed gas molecules (SO2, H2S, SOF2, SO2F2 and CF4) on Pd-doped (8, 0) SWCNTs was explored through density functional theory-based method. The geometrical and electronic structures, density of state and frontier molecular orbital were analyzed to predict the adsorption properties and mechanism of complexes.
In the adsorption of SO2, strong binding energy between SO2 and Pd-SWCNTs indicates the nature of chemical adsorption. The adsorption energy increases with the rise of SO2 molecule number adsorbed on Pd-SWCNTs. The large contribution of SO2 and the total DOS near the Fermi level is responsible for the conductance increase of SO2-Pd-SWCNTs. The high adsorption sensitivity of Pd-SWCNTs makes it suitable for SO2 detection.
For the adsorption SOF2, F-end adsorption conformation is energetically favorable. The large formation energy and structure change show that the SOF2 molecule is chemically bonded to Pd-doped SWCNTs. The large enhancement toward the Fermi level induced by the LDOS of SOF2 implies the increase of conductance for the SO2-Pd-SWCNTs. However, the strong repulsive force between the SOF2 molecules limits it is further adsorption, and therefore, the increased conductivity introduced by SOF2 is smaller than SO2.
Upon the adsorption of one SO2F2 to the Pd-SWCNTs, the HOMO-LUMO energy gap of the SO2F2-Pd-SWCNTs increased to 0.415 eV, which is larger than that of the Pd-SWCNTs, whereas the TDOS at Fermi level slightly decreased. The command action of the HOMO-LUMO energy gap and TDOS finally led to the conductivity decrease of the SO2F2 adsorbed Pd-SWCNTs.
When CF4 is adsorbed on Pd-SWCNTs, the HOMO-LUMO energy and TDOS remained unchanged based on our computation. The Pd-CNT showed low sensitivity for CF4 gas.
Results of the theoretical calculation showed that Pd-SWCNTs had different sensitivity to the SF6 decomposition gases. After SO2, H2S and SOF2 were adsorbed on Pd-SWCNTs, the conductivity increases in the following order: SO2 > SOF2 > H2S. The conductivity of SO2F2 decreased when it was adsorbed by Pd-SWCNTs. Conversely, Pd-SWCNTs are not sensitive to the other gas molecule CF4. Through changes in conductivity, the Pd-SWCNTs achieved selective detection of five SF6 decomposition gases: SO2, H2S, SOF2, SO2F2 and CF4.
2.4. Gas-sensing properties of Ni-SWCNTs to SOF2, SO2F2, SO2, H2S, HF, CF4 and SF6
2.4.1. Structural parameters of intrinsic Ni-SWCNTs
After an individual Ni atom was decorated onto the SWCNTs and relaxed to stable structure, the Ni atom distinctly protruded out of the SWCNTs sidewall due to the large Ni atom radius compared with that of SWCNTs as shown in Figure 23 . The bond length C3-Ni was stretched to 1.84 Å, and the bond length C4-Ni length along the axial of Ni-SWCNTs increased to 1.76 Å.
2.4.2. The analysis of gas adsorption structure
After the optimization of individual Ni-SWCNT and gas molecules, the gas molecules were relaxed to various sites on the surface of Ni-SWCNTs to get the lowest energy structure . Moreover, in order to fully analyze the influence brought by decomposed products, adsorption of both single and double gas molecules was studied in this work . As seen in Figure 24, it was found that all of the gas molecules intended to be adsorbed at the Ni-doped site, which acted as an active site for adsorption . To analyze the adsorption properties, the banding distance
As shown in Table 4 and Figure 24a–c, single SO2, SOF2 and SO2F2 molecules were adsorbed onto SWCNTs. The oxygen atoms of both SO2 and SOF2 were close to the Ni atom with the nearest bond length of 2.00 and 2.06 Å because of the strong electronegativity of oxygen atom . And the sulfur atom was further away from the Ni-SWCNTs sidewall because it built a stable covalent bond with oxygen atoms and fluorine atoms, making it hard to interact with the Ni atom . The structures of SO2 and SOF2 were almost kept unchanged in the adsorption process. The low
As to the adsorption of two identical gas molecules, as seen in Table 4 and Figure 24d–f, the double SO2 adsorption was similar to that of single SO2 molecule with a nearest bond length of 1.97 Å . Interestingly, the structures of both SOF2 molecules were deformed with two new SOF molecules produced in the adsorption process, indicating that the Ni-doped metal showed great adsorption ability . According to the SO2F2 adsorption, one of the SO2F2 molecules deformed to one SO2 and two fluorine atoms that were adsorbed on Ni atom . And the other SO2F2 molecule was close to the Ni atom with a binding distance of 2.29 Å . The
As for the adsorption of two foreign gas molecules on Ni-SWCNTs shown in Table 4 and Figure 24g–i, there was no significant difference in the adsorption length for SO2 compared with that of single and double SO2 adsorption in Figure 24a and d. It should be noticed that the molecule structures of SOF2 (Figure 24g) and SO2F2 (Figure 24h) kept unbroken, while in the SOF2 and SO2F2 case in Figure 24i, one fluorine broke up from SO2F2 and was adsorbed on the Ni atom, and the SOF2 molecule was away from the sidewall of Ni-SWCNTs with an adsorption length of 3.61 Å.
2.4.3. The analysis of the density of states and frontier molecular orbital
188.8.131.52. Adsorption of single decomposed gas molecule on the surface of Ni-SWCNT
According to the detection mechanism of chemiresistor sensor, the conductivity of gas-sensing materials changes in response to the different gas molecules . Using the density of states (DOS) and frontier molecular orbital theory, the factors influencing the change of conductivity can be found directly . We first analyze the single gas molecule adsorption cases, including SO2, SOF2 and SO2F2 (Figure 24a–c). Along with the charge transfer between the gas molecules and Ni-SWCNTs, the total density of states (TDOS), the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) were distinctly changed . If the energy gap between HOMO and LUMO narrows down, the charge carrier transfer becomes easier from HOMO to LUMO. Then, the conductivity of adsorption system increases correspondingly .
The continuous TDOS of Ni-SWCNTs shown in Figure 25a is consistent with the verified results that intrinsic Ni-SWCNTs possess good conductivity after Ni atom doping. Bak et al. reported that mesoporous nickel/CNTse hybrid material showed high conductivity . Comparing TDOS before (Figure 25a) and after (Figure 25b) the SO2 molecule adsorption on the surface of Ni-SWCNTs, there is no significant change of TDOS at the energy levels that are far below or far above the Fermi level, and the main change is located at the energy level that is slightly above the Fermi level, which is attributed to the SO2 adsorption that increases the number of effective charge. For the case with SOF2 molecule adsorption, the TDOS almost does not change below the Fermi level as shown in Figure 25c. Although the TDOS far above the Fermi level slightly increases, it has no contribution to the change of conductivity, which agrees with the low interaction energy discussed above. For the adsorption of single SO2F2 (Figure 25d), the TDOS increases below the Fermi level and decreases above the Fermi level due to the chemisorption.
The HOMO, LUMO,
184.108.40.206. Adsorption of double identical decomposed gas molecule on the surface of Ni-SWCNT
In practical situation, the insulated SF6 gas may simultaneously decompose to SO2, SOF2 and SO2F2, indicating that it is mixed gas in SF6 insulated equipment. Therefore, the multiple gas molecule adsorption was considered in our study. With the limited adsorption ability of single Ni-doped SWCNTs, double gas molecule adsorption is sufficient to analyze the situation of multiple gas molecule adsorption. The influence on conductivity brought by absorption of double identical decomposed gas molecules is discussed first. Comparison of the TDOS before and after gas molecule adsorption is shown in Figure 27. The presence of Ni active site leads to double identical SO2 simultaneously adsorbed on Ni-SWCNTs, resulting in an enhancement of the communization movement between the Ni-SWCNTs and adsorbed gas molecules. As can be seen form Figure 27a and b, the TDOS was improved in all energy distribution zone, although the TDOS just above the Fermi level changed little, but that below the Fermi level increased, which means that the major carrier transfer from the valence band and the conduction band is enhanced. When the double identical SOF2 and SO2F2 molecules interacted with Ni-SWCNTs by chemisorption, the TDOS near the Fermi level reduced. It can be seen in Figure 27c, the decrease area of TDOS for SOF2 adsorption is slightly below the Fermi level, while a sharp TDOS reduction occurs above the Fermi level for SO2F2 adsorption as shown in Figure 27d.
Table 6 presents the results of the LUMO and HOMO energies of the double identical SF6 decomposed products (SO2, SOF2 and SO2F2) adsorption on the surface of Ni-SWCNTs based on DFT calculation. All of the energy of HOMO and LUMO declined during the adsorption process. Considering the distribution of frontier molecular orbital for double SO2 physisorption in Figure 28b1 and 6b2, the HOMO evenly distributed on the structure of Ni-SWCNTs. In addition, the
220.127.116.11. Adsorption of double foreign decomposed gas molecule on the surface of Ni-SWCNT
In case of mixed gas decomposed in SF6 insulated equipment, the mixed gas molecules could also be adsorbed on the surface of Ni-SWCNTs with double foreign gas molecules except the double identical adsorption case discussed above. According to the TDOS shown in Figure 29, the change of TDOS presents significant difference comparing with that of single and double identical gas molecules adsorption. All of the TDOS near the Fermi level has increased. As discussed in the geometry analysis for SO2&SOF2 adsorption, both gas molecules move close to the surface of Ni-SWCNTs by physisorption. The sharply increased TDOS above the Fermi level (see Figure 29b), which is even bigger than that of single SO2 adsorption implies the prominent improvement of conductivity. And the change of conductivity is agreed with the literature that reported the increase of conductivity during SO2 gas detection . When SO2&SOF2 interacted with Ni-SWCNTs, the SOF2 molecule was away from the surface of Ni-SWCNTs according to the structure discussed before. Comparing the TDOS of SO2&SO2F2 adsorption (Figure 29c) with that of single SO2, we found that the change of TDOS presents identical increase trend, deriving from the crucial role of SO2 adsorption. For the adsorption of SOF2&SO2F2, only the broken fluorine atom and one SOF2 made contribution to the change of conductivity. As the TDOS of SOF2&SO2F2 adsorption depicted in Figure 29d, the TDOS near the Fermi level and site of the HOMO and LUMO increased.
All of the increased TDOS for mixed gas molecule adsorption is consistent with the frontier molecular orbital analysis in Figure 30. It can be seen obviously that the HOMO and LUMO distribution (see Figure 30b and Table 7) has extended to the surface of adsorbed SO2 and SOF2molecules, and the
2.4.4. Summary: gas adsorption on Ni-SWCNTs
In summary, the adsorption effects of typical decomposition products: SO2, SOF2 and SO2F2 in SF6 insulated equipment toward Ni-doped (8, 0) zigzag SWCNTs have been theoretically investigated using first-principle calculation based on PBE function of DFT. It is found that the gas molecules tend to approach the surface of Ni-SWCNTs at the Ni-doped active site with the improved adsorption ability to gas molecules. The density of state and frontier molecular orbital were adopted to study the physical properties of Ni-SWCNTs before and after gas molecules adsorption. Comparing the change of conductivity in different adsorption situations, the conductivity of Ni-SWCNTs increases in the following order: SO2 > SOF2 after SO2 and SOF2 adsorbed onto Ni-SWCNTs. Conversely, SO2F2 adsorption onto Ni-SWCNTs slightly decreases conductivity. The following specific conclusion can be drawn.
For single decomposed gas molecule adsorption, SO2 and SOF2 interact with Ni-SWCNTs via physisorption, while SO2F2 strongly chemisorbed on Ni-SWCNTs. For SO2 adsorption, the TDOS near the Fermi level and the HOMO and LUMO increases with a declined
For the adsorption of double identical gas molecules, the double SO2 is still physically adsorbed on Ni-SWCNTs, and the chemisorption acts on both SOF2 and SO2F2. Considering the conductivity features, we conclude that the double SO2 molecules increase the conductivity, while double SOF2 and double SO2F2 adsorption show a decrease effect to conductivity.
The results of gas-sensing properties to mixed gas molecule adsorption have showed that the conductivity increases at different extent, reflecting the sensing specific to different gas molecules. In case of SO2 and SOF2 and SO2 and SO2F2 adsorption, the improvement of conductivity is mainly derived from the contribution of SO2 adsorption, which has also been founded in single and double SO2 adsorption. For SOF2 and SO2F2 adsorption, the Ni active site bonded with a fluorine broke form SO2F2 and the other two SOF2 molecules away from the surface of Ni-SWCNTs, resulting in the increase of conductivity due to the evenly distributed LUMO.
Taking advantage of the sensing mechanism of Ni-SWCNTs to SF6 decomposed products: SO2, SOF2 and SO2F2, the Ni-SWCNTs gas chemiresistor sensor can be prepared to realize the online detection and diagnosis of insulated faults in SF6 insulated equipment.
2.5. Gas-sensing properties of Al-SWCNTs to SOF2, SO2F2, SO2, H2S, HF, CF4 and SF6
2.5.1. Structural parameters of intrinsic Al-SWCNTs
When a carbon atom C1 was substituted by an Al atom, significant geometric changes occurred in Al-SWCNTs, as shown in Figure 31. Considering that the radius of the Al atom is larger than that of the carbon atom, the Al heteroatom protruded from the Al-SWCNT surface after structural optimization . The bond length between Al─C3 and Al─C4 atoms reached 1.908 and 1.841 Å, respectively. The calculation results were similar to that of other research [17, 32, 33].
2.5.2. The analysis of gas adsorption structure
Following the optimization of each initial structure, all gas molecules were allowed to relax on the surface of Al-doped SWCNTs . Cause the orientational effects play important role on the adsorption results. In addition, in order to receive the global minimum-energy structures from the all these minimum-energy structures, which may contain some local minimum-energy structures. Various adsorption sites and approaching ways of decomposition products were calculated to get the most minimum-energy structures, which are used as the most stable structure for each gas molecule adsorption in our study (Figure 32) . The results showed that all of the gas molecules tended to adsorb at the site of Al atom, which revealed the stronger adsorption of Al atom than other undoped sites. Given that the electrical properties of SWCNTs could be significantly influenced by gas adsorption [32, 34], the strong adsorption provided an opportunity for the detection of SF6 decomposition products based on the change of conductivity .
The adsorption energy
As shown in Figure 32a1 and a2 and Table 8 , when one SO2 molecule approached the surface of Al-SWCNTs in a different direction, two oxygen atoms were close to the Al atom. Meanwhile, the sulfur atom is far from the Al atom because the sulfur atom has already built a strong double bond with adjacent oxygen atoms. This steady interaction does not allow the sulfur atom to form another coordinate bond with the Al atom. The bond distance and angle of the SO2 molecule slightly changed during the adsorption process, which corresponded with the result of a previous study [32, 36]. In the present study, the interaction distance between SO2 molecule and Al atom was 1.988 Å, which is slightly smaller than that of Pd-doped (8, 0) SWCNTs  because the radius of the Al atom is smaller than that of the Pd atom . Long gas interaction distance (1.988 Å) and low banding energy (−1.606 eV) indicated that the adsorption was some type of physisorption [32, 38]. When the second SO2 molecule was adsorbed on Al-SWCNTs, the SO2 molecules approached the Al atom with only one oxygen atom because of the repulsive interaction between the two gas molecules. The adsorption energy increased to 2.206 eV, with adsorption distances of 1.787 and 1.868 Å to the Al atom .
The adsorption structures and parameters of single and double H2S molecules on Al-SWCNTs are shown in Figure 32b1 and b2 and Table 8 . After the relaxation process, a quasi-tetrahedron geometry around the Al center was observed. The hydrogen atoms and sulfur atom in the H2S molecule generated strong bond energy . Thus, the interaction between hydrogen atoms and Al was weak. Meanwhile, the sulfur atom could still react with the Al atom because of its multivalent feature. As such, the H2S molecule approached the Al atom through the sulfur atom. The interaction distance between the S and Al atoms was approximately 2.47 Å, with the H─Al distance of 2.85 Å . Considering the long interaction distance and low binding energy of −1.051 eV, the interaction indicated a moderate physisorption. When double H2S molecules adsorbed on the surface of Al-SWCNTs, we observed that one molecule was distinctly far from the surface with a distance of 3.495 Å because of the repulsive force between molecules . However, the adsorption site of the other H2S molecule changed slightly compared with the former single molecule adsorption. The distance from the new added H2S molecule to the doped Al atom was approximately 2.425 Å. The binding energy between single H2S and Al-SWCNTs was approximately −1.051 eV, whereas the binding energy between double H2S and Al-SWCNTs increased to −1.498 eV . The Mulliken population analysis indicated that 0.234 and 0.273 electrons transferred from single and double H2S molecules to Al-SWCNTs, respectively. In addition, our results were similar to the results of previously studied Au-doped SWCNTs [32, 40], in which the structural parameters, binding energy and charge transfer were also reported. Small difference between our results and than in previous report was found probably because different models were used in the calculations. Al-SWCNTs can be considered a possible sensor material for the detection of H2S owing to the adsorption energy and considerable charge transfer .
Based on the optimized adsorption structures of SOF2 shown in Figure 32c1 and c2 and Table 8 , two types of adsorption, namely single and double SOF2 molecule adsorption, were outlined to analyze the adsorption capacity. From the relaxed structure of single SOF2 molecule adsorption, the strong interaction between SOF2 molecule and Al-SWCNTs decomposed the SOF2 molecule to one SOF molecule and another fluorine atom . The electronegative fluorine atom bonded to the Al atom through a strong chemical reaction, with the interaction distance of 1.699 Å. Meanwhile, the bond length from the produced SOF molecule to the fluorine atom was 2.777 Å, which indicated the decomposition of SOF2 . Upon double SOF2 molecule adsorption, one of the SOF2 molecules was adsorbed on the surface of Al-SWCNTs by chemisorption , whereas the other SOF2 molecule was found far from the nanotube . Two of the original Al─C bonds broke in the adsorption process. Then, two fluorine atoms of SOF2 bonded to the Al atom .
As shown Figure 32d1 and d2 and Table 8 , single and double SO2F2 molecules are adsorbed on the surface of Al-SWCNTs. After the structures have relaxed to reach the most steady state, only one original Al─C bond exists after the adsorption process. The other two bonds were broken because of the strong interaction between the F and Al atoms [32, 41]. Upon single SO2F2 molecule adsorption, two fluorine atoms separated from SO2F2 molecule and bonded to the Al atom, with bond lengths of 1.679 and 1.695 Å, respectively. Meanwhile, the produced SO2 molecule was far from the surface of Al-SWCNTs. When another SO2F2 molecule was added, all of the fluorine atoms separated from the SO2F2 molecules. Three of the fluorine atoms bonded to the Al atom. The other fluorine atom bonded to the carbon atom of Al-SWCNTs. Both of the produced SO2 molecules were far from the surface of Al-SWCNTs, with interactive distances of 2.589 and 3.410 Å, respectively. The weak interaction to the produced SO2 might be because the Al-SWCNTs have reached saturated adsorption .
As shown in Figure 32e1 and e2 and Table 8 , the CF4 molecule was far from the surface of Al-SWCNTs, which was also ineffectively detected by other reported methods . The nearest interaction distances reached 3.27 Å for single CF4 molecule adsorption and 2.710 and 2.537 Å for double CF4 molecule adsorption. The long interactions corresponded well with the low adsorption energies of −0.033 and −0.087 eV for single and double CF4 molecule adsorption, respectively. Furthermore, weak physisorption was consistent with slight charge transfer .
2.5.3. The analysis of the density of states and frontier molecular orbital
In the previous section, we discussed the adsorption of single and double SF6 decomposed gas molecules on Al-SWCNTs. We observed that the Al doping method showed good adsorption capacity for all of the SF6 decomposed gas molecules, except for the CF4 molecules, which indicated the possibility of detecting these decomposition components . However, the detecting mechanism of Al-SWCNTs depends on its conductivity change after gas adsorption. The density of states (DOS) and frontier molecular orbitals were investigated to analyze the change of conductivity. The total electron DOS (TDOS) and local DOS (LDOS) were determined to investigate the influence of gas adsorption and to elucidate the electronic properties of Al-SWCNTs and molecule-Al-SWCNTs [32, 43], as shown in Figure 33. The highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) upon molecule adsorption on the Al-doped SWCNTs are listed in Table 9. The corresponding diagrams of HOMO and LUMO are shown in Figure 34 .
|System||EHOMO (eV)||ELUMO (eV)||Eg (eV)|
Based on the DOS of SF6 decomposition products before and after adsorption (Figure 33) , we observed that the LDOS of the Al atom had only a slight contribution to each TDOS. The changes of TDOS were mainly from the adsorbed molecules. Meanwhile, the various changes induced by different adsorbed molecules only provided the chance to detect the SF6 decomposition products selectively .
Based on Figure 33a1 , the TDOS of Al-SWCNTs was apparently distributed to all energy band areas, which reached 4.43 eV at the Fermi level. This finding indicated that Al-SWCNTs are still a good conductor after Al atom doping. The results are in accordance with other experiments on metal-doped materials . Figure 33a1 and a2 shows the frontier molecular orbitals of Al-SWCNTs. In addition, the HOMO and LUMO were uniformly located on the Al-SWCNT surface. The HOMO and LUMO of the Al atom were mainly contributed by its
The TDOS for SO2 molecules adsorbed on Al-SWCNTs is shown in Figure 33b1 and b2 . When one SO2 molecule was adsorbed on the surface of Al-SWCNTs, the TDOS slightly increased at and under the Fermi level compared with that of pristine Al-SWCNTs. As shown in Figures 22b2 and 33b1, the HOMO and LUMO were entirely located on the carbon atoms upon single SO2 adsorption. The HOMO energy shifted from −5.077 to −5.292 eV, and the LUMO energy shifted to −5.030 eV in the pristine Al-SWCNTs.
As shown in Figure 33c1 and c2, the LDOS induced by the H2S molecules was partly located above the Fermi level, which contributed to the TDOS above the Fermi level. The change of the HOMO and LUMO energies slightly shifted to the right side.
Based on the SOF2 molecules adsorbed on Al-SWCNTs shown in Figure 33d1 and d2, the LDOS of SOF2 molecules was mainly below the Fermi level. Herein, the TDOS at the Fermi level was slightly changed compared with that of pristine Al-SWCNTs. However,
When one SO2F2 molecule was adsorbed on Al-SWCNTs, the TDOS decreased around the Fermi level (Figure 33e1). The LDOS of SO2F2 was primarily below the HOMO energy and above the LUMO energy, with the decrease in
As mentioned previously, the interaction between CF4 molecules and Al-SWCNTs was weak, resulting in a limited influence of the CF4 molecules . The LDOS of CF4 was below the HOMO energy shown in Figure 33f1 and f2 . Meanwhile, the TDOS around the Fermi level remains unchanged.
2.5.4. Summary: gas adsorption on Al-SWCNT
In this study, we analyzed the adsorption of the gases produced by SF6 decomposition (i.e., SO2, H2S, SOF2, SO2F2 and CF4) on the Al-SWCNT surface using GGA and DFT calculations and considering different sites to determine the most stable structures. In addition, multiple-molecule adsorption was calculated for SF6 decomposition products to analyze the various changes of conductivity induced by adsorption .
The results indicated that the SO2 molecules were physically adsorbed on Al-SWCNTs. This interaction increased the TDOS and decreased the
In summary, Al atom doping method is potentially an effective technique to adsorb the gases produced by SF6 decomposition. Through the different changes in conductivity induced by molecule adsorption, the selective detection of each type of SF6 decomposed gas was achieved. We hope that this innovative study would further accelerate research on the mechanism of metal doping methods in detection of gases from SF6 decomposition .
2.6. Gas-sensing properties of Pt-SWCNTs to SO2, H2S
2.6.1. Structural parameters of intrinsic Pt-SWCNT
The radius of Pt atom is 0.183 nm, which is greater than that of C atom (0.070 nm). Thus, Pt is highlighted on the CNT surface as shown in Figure 35. The bond lengths between Pt atom and three adjacent C atoms changed from 0.142 nm to 0.199, 0.199 and 0.189 nm for Pt-C1, Pt-C2 and Pt-C3, respectively . These results are consistent with Refs. [16, 46].
2.6.2. The analysis of gas adsorption structure
Pt is not only a sensing element of Pt-SWCNTs, but also an active site. Strong interaction with gas molecules adsorbed on the surface results in deformation of Pt-SWCNTs and elongation of Pt-C bond. The full geometric optimization of the Pt-SWCNTs and SO2 adsorption model is shown in Figure 36. An oxygen atom O1 points to Pt, in which the distances of Pt-O1 and Pt-S are 0.212 and 0.245 nm, respectively.
The reaction adsorption energy for SO2 adsorption is −1.225 eV, which denotes an exothermic and spontaneous reaction. According to Mulliken charge population analysis shown in Table 10, SWCNTs of Pt-SWCNTs have 0.147 positive charge, and Pt has 0.147 negative charge before adsorption. After the adsorption process, SWCNTs have 0.509 positive charge, whereas Pt has 0.116 negative charge. SO2 obtains 0.301 electrons during the adsorption reaction . Charge variation (Δ
As shown in Table 10 , Mulliken charge analysis shows that H2S donates 0.285 electrons. Pt and SWCNTs, respectively, have 0.019 and 0.266 electrons after H2S is adsorbed on Pt-SWCNTs. A large number of electron transformations convert Pt-SWCNTs from
2.6.3. The analysis of the density of states and frontier molecular orbital
The transfer of a large number of electrons during adsorption causes the redistribution of system charges. The density of states (DOS) near Fermi level appears impure state, and the DOS between HOMO and LUMO changes. Figure 37 shows that these impure states are caused by SO2 adsorption. The
SO2 adsorption on the surface of Pt-SWCNTs has large adsorption energy and can form a stable structure. The
The adsorption reaction of Pt-SWCNTs and H2S is also exothermic, with
2.6.4. Summary: gas adsorption on Pt-SWCNTs
In this study, adsorptions of three gases on the surface of Pt-SWCNTs were calculated based on DFT . The gas-sensing properties of Pt-SWCNTs were assessed according to the changes in adsorption energy, geometric structure and electronic structure during adsorption. The main conclusions are as follows :
The three adsorption reactions are exothermic and spontaneous.
The adsorption energy of the reaction between Pt-SWCNTs and SO2 is large, and numerous electrons are transferred from CNTs to the target gases . The frontier orbital energies (
H2S is reduced when reacted with Pt-SWCNTs and provide a large number of electrons, thereby converting CNTs from
Results of the theoretical calculation show that Pt-SWCNTs can respond to the three gases . The electrical characteristics of Pt-SWCNTs show different degrees of changes after adsorption of the test gases. As SO2 is adsorbed on Pt-SWCNTs, CNT loses electrons, hole carriers are increased and conductivity is enhanced . As H2S is adsorbed on the surface of CNTs, Pt-SWCNTs receive a large number of electrons and transforms from
2.7. Gas-sensing properties of Au-SWCNTs to SO2, H2S
2.7.1. Structural parameters of intrinsic Au-SWCNTs
The radius of the Au atom is significantly greater than that of the C atom; thus, the Au atom of Au-SWCNT is highlighted on the nanotube surface shown in Figure 41 . The bond lengths between the Au atom and the three adjacent C atoms are 0.207 (Au─C1), 0.208 (Au─C2) and 0.196 nm (Au─C3). Compared with the C─C bond length of the intrinsic structure, the Au─C bond lengths are elongated by 38, 38 and 46%, respectively .
2.7.2. The analysis of gas adsorption structure
The adsorption structures of the gas molecules adsorbed by Au-SWCNT in different initial positions were calculated. We chose two initial positions that are parallel to the nanotube axis and three initial positions that are perpendicular to the nanotube axis. The initial positions were optimized in the geometrical structure . During observation of the optimized structures, the stable adsorption structure of H2S is the S atom located above the center of the ring that contains Au─C1─C2 . Two main stable adsorption structures of SO2 exist. One is the S atom located above the Au─C bond and an O atom above the center of the ring that contains Au─C1─C2; another is the S atom located above the center of the ring . SO2 that is parallel to the axis, and two O atoms above the Au and C atom, respectively. Comparing the two structures, the former is more stable. The most stable adsorption structure is shown in Figure 42. Table 11 lists the adsorption energy and the structural parameter .
The adsorption energy of SO2 is −1.258 eV, which indicates that the adsorption is exothermic and spontaneous. After SO2 is adsorbed to Au-SWCNT, the structures of Au-SWCNT (Table 11) and SO2 (Figure 42) changed . Au─C1 and Au─C2 are elongated by 3.38 and 4.33%, respectively. Moreover, S─O is also elongated. The modified element of CNT is the sensing element and the active site of the modified CNT . The adsorption partially depends on the interaction between the gas molecule and the sensing element. The strong attraction in the adsorption of SO2 and Au-SWCNT caused the structural change of Au-SWCNT . The Au─C bond length increased, the bond energy decreased, and the bond activity strengthened. Simultaneously, the electrons are transferred to SO2, and the excess electrons fill the anti-bonding orbits of SO2. The increase in repulsion results in a change in the S─O bond length from 0.148 nm to 0.150 and 0.160 nm .
The adsorption between H2S and Au-SWCNT is also exothermic, and the adsorption energy is −1.317 eV. Compared with SO2, the interaction is slightly stronger. Au─C1 and Au─C2 are elongated by 4.83 and 4.81%, respectively .
From the above analysis, Au-SWCNT has a strong adsorption with SO2 and H2S, and their adsorption energies are greater than 1 eV. The adsorption reaction can occur at room temperature and the strong interaction changes the geometric structure of the adsorption system .
2.7.3. The analysis of the density of states and frontier molecular orbital
In Table 12 , the LUMO of SO2 was approximated to the HOMO of Au-SWCNT, and the difference of the two orbital energies is only 0.065 eV. The electron of Au-SWCNT only needs to cross a very low energy barrier to transfer to SO2. In turn, the electron needs to cross a 3.603 eV energy barrier for the electron of SO2 to transfer to Au-SWCNT, but this process is more difficult . Thus, the electrons transfer from Au-SWCNT to SO2 during adsorption. According to Mulliken charge population, SO2 obtains 0.301 electrons during the adsorption reaction. SWCNT and Au lose 0.269 and 0.032 electrons, respectively. Au has a key role in the adsorption reaction. Figure 43 shows the three-dimensional plot of the deformation electron density of SO2-Au-SWCNT . The range is from −0.976 to 0.345 e/nm. The negative value denotes loss of electrons and a decrease in the electron density. The positive value denotes gain of electrons and an increase in the electron density. As seen from the plot, the charge of Au-SWCNT was redistributed after it adsorbed SO2. SO2 obtained electrons, whereas Au-SWCNT lost electrons. Correspondingly, the HOMO and LUMO move toward the nuclear and the orbital energy decreases. Au-SWCNT is a p-type semiconductor. The transferred electrons increased the electron holes and simultaneously increased the carriers, enhanced the conductivity, and decreased the frontier orbital energy gap (Table 12) .
To clarify further the adsorption processes of SO2, the partial density of states (PDOSs) of the S, O and Au atoms are shown in Figure 44 . Their PDOSs overlap in the energy region of −10 to −2.5 eV. In this area, the d orbitals of Au, the p orbitals of the S and O atoms are hybridized as the molecular orbitals of the system. In addition, the d orbitals of Au and the p orbitals of S effectively overlap at the Fermi energy (−2.5 eV to 2.5 eV), which strengthens the interaction between the two atoms. The hybridized orbitals at the Fermi level introduce an impurity level and are conducive for the electrons to transfer to SO2 from Au-SWCNT .
Based on the changes in the electronic structure of adsorption system, a significant amount of electrons is transferred in the adsorption process between SO2 and Au-SWCNT. Au-SWCNT loses electrons, the frontier orbital energy gap decreases, and the conductivity is enhanced. In conclusion, the Au-SWCNT has a good sensitivity to SO2 and can be used to detect SO2 gas based on the changes in its conductivity .
The S of H2S is at the lowest valence state. It has a strong reducibility and can provide electrons during the reaction process. In contrast to SO2, the HOMO of H2S was approximated to the LUMO of Au-SWCNT, and the difference of the energy is only 1.304 eV. Therefore, the electrons of H2S are easily transferred to Au-SWCNT. Transferring the electrons of Au-SWCNT to H2S is difficult. Thus, when H2S was adsorbed to Au-SWCNT, the electrons were transferred from H2S to Au-SWCNT . According to the Mulliken charge population, the H2S molecule loses 0.286 electrons. The SWCNT and the Au atom obtain 0.176 and 0.110 electrons, respectively. The three-dimensional plot of the deformation electron density of H2S-Au-SWCNT is shown on Figure 45 . The range is −1.172 to 0.320 e/nm. The charges of Au-SWCNT and the adsorbed H2S are redistributed, H2S loses electrons and Au-SWCNT gains electrons. Correspondingly, the HOMO and LUMO of Au-SWCNT move away from the nucleus and the orbital energy increases. The transferred electrons decreased the number of electron holes, along with the number of carriers and the conductivity. The frontier orbital energy gap also increased (Table 12) .
When observing the PDOSs of the adsorption system shown in Figure 46 , which is similar to that of SO2, the PDOSs of Au in Au-SWCNT and S in H2S are overlapping. The d orbitals of Au and the p orbitals of the S atom are hybridized, which is advantageous to the electron transfer and strengthens the interaction between the adsorbed H2S and Au-SWCNT.
Therefore, Au-SWCNT has a good sensitivity to H2S, and H2S can be effectively adsorbed on the surface of Au-SWCNT . When the Au-SWCNT acquired electrons, the frontier orbital energy gap increased, and the conductivity decreased. Hence, Au-SWCNT can be used to detect H2S .
2.7.4. Summary: gas adsorption on Al-SWCNTs
In this study, the adsorption reactions of the two gases on the surface of Au-SWCNT were calculated by DFT, and the sensitivity of Au-SWCNT to the two gases was analyzed .
The main conclusions of this study are as follows:
The reactions between the two gases and Au-SWCNT are both exothermic, and the adsorption energies are huge. The interaction between the gas molecule and the nanotubes caused the structure to change, for example, Au─C elongate .
During the adsorption process of SO2, SO2 acquires electrons and Au-SWCNT loses electrons. The frontier orbital energy gap decreases, and the electrical conductivity of p-type Au-SWCNT is enhanced.
During the adsorption process of H2S, H2S loses electrons and Au-SWCNT acquires electrons. The frontier orbital energy gap increases, and the electrical conductivity of p-type Au-SWCNTs decreases.
The theoretical calculation results show that Au-SWCNT has a good sensitivity to both SO2 and H2S . The conductivity changes caused by the two gases are inversely proportional. Thus, Au-SWCNT can be used to detect SO2 and H2S . This conclusion is helpful to the development of CNT-based gas sensors and provides a theoretical basis for developing Au-SWCNT-based gas sensor .