Highly Efficient MoS2/CsxWO3 Nanocomposite Hydrogen Gas Sensors

Introduction

A polluted atmosphere endangers the health of living organisms. It comprises various gases that exist in nature and those released from industries (Masteghin et al., 2019; Pisarkiewicz et al., 2020; Duc et al., 2020; Kim et al., 2021). These odorless, tasteless, colorless gases are toxic when they exceed the safe limits (Ha et al., 2018; Miglietta et al., 2020; Pisarkiewicz et al., 2020). Hydrogen (H₂), carbon dioxide (CO₂), carbon monoxide (CO), and ammonia (NH₃) present in the environment have adverse effects on human health when their concentrations exceed the permissible levels (Annanouch et al., 2021; Hübert et al., 2014; Saravanan et al., 2017). Therefore, the amount of these gases in the environment must be monitored, and the development of effective and efficient detection methods is essential.

Hydrogen is one of the most hazardous gas and regulating its concentration with adequate monitoring devices is crucial (Hübert et al., 2014). Currently it is extensively used as a major ecological energy source and is used in semiconductor processing, chemical industry, nuclear reactors, and petroleum extraction. Hydrogen is a potential candidate for next-generation energy requirements in power plants, automobile transportation, and aerospace industries. However, the storage and regulated supply of hydrogen are challenging owing to the potential dangers of leakage (Saravanan et al., 2017). Therefore, developing long-lasting and cost-effective hydrogen sensing devices that are highly reliable for the accurate detection of the hazardous hydrogen gas is compelling (Hienuki et al., 2021; Liang et al., 2021; Sridhar et al., 2021).

In recent years, tungsten-based materials have gained a lot of interest owing to their nanostructures and unique chemical and physical properties (Chala et al., 2017; Motora and Wu, 2020; Wu et al., 2019). Because of their good selectivity and stability, they are the most suitable for fabricating high-grade sensors. In particular, tungsten trioxide has been extensively used in sensors for the detection of hazardous gases, such as hydrogen, ammonia, nitrous oxide, and hydrogen sulfide (Wang et al., 2000; Rydosz et al., 2014; Castillo et al., 2020; Dong et al., 2020). However, most of the WO₃-based gas sensors function at high temperatures or have high response/recovery times, which hinder their practical application (Esfandiar et al., 2014; Chang et al., 2020). Therefore, the development of tungsten oxide-based gas sensor materials that can circumvent these limitations is important. In our previous study, we proposed a new tungsten bronze material-cesium tungsten oxide (Cs_xWO₃) for hydrogen gas sensors, which exhibited significant hydrogen gas sensing properties at room temperature owing to its mixed-valence state and unique properties (Wu et al., 2021). However, its sensor response and response time need to be enhanced to detect hydrogen gas within a short duration, which are crucial for practical applications. Therefore, to circumvent this limitation, a suitable sensor material should be selected.

In contrast, molybdenum disulfide is a transition metal dichalcogenide (TMD), which is used in various applications, such as photocatalysis, sensing, disinfection, contaminant adsorption, and membrane-based separation (Barua et al., 2017; Li et al., 2018; Bello et al., 2020). It has been applied in the field of sensors as photochemical sensors, gas sensors, glucose sensors, photodetectors, electrochemical sensors, and DNA sensors (Zhang et al., 2015; Akbari et al., 2018). Among the different types of gases, MoS₂ nanostructures are usually selective toward NH₃ gas at room temperature, which hinders their applicability as gas sensors. Although MoS₂ is a good sensing material, it has limitations, such as a low structural strength and conductivity (Huaning et al., 2021). However, few studies have shown that its selective behavior can change while forming hybrids with different materials; this can be ascribed to the charge-transfer-based modulation of the channel conductivity of the gas sensor mechanism (Gottam et al., 2020). Therefore, combining MoS₂ with unique material is important for achieving an enhanced sensing performance. For instance, WO₃/MoS₂ composites have been developed, and the nanocomposite exhibits excellent ammonia and hydrogen sulfide sensing properties (Singh et al., 2020, Singh et al., 2021). However, these sensor devices function only at temperatures higher than 200°C. Besides, most of the previously developed hydrogen gas sensor exhibited low sensor response. It is very important to develop hydrogen gas sensor with high sensitivity, selectivity, and stability for practical applications. Therefore, the development of MoS₂ composites with excellent hydrogen sensing performance at room temperature is crucial.

Herein, we developed Cs_xWO₃@MoS₂ nanocomposites for application in hydrogen gas sensors through a solvothermal method by taking advantage of the low-temperature sensing properties of Cs_xWO₃ and the high sensor response of MoS₂. The hydrogen gas sensing properties of the developed Cs_xWO₃@MoS₂ nanocomposite gas sensor at room temperature were systematically investigated. The proposed gas-sensing mechanism of the sensor was also explained.

Materials and Methods

Materials

The tungsten hexachloride (WCl₆), cesium hydroxide (CsOHH₂O), anhydrous ethanol, and acetic acid were purchased from Kanto Chemical Co., Inc. Molybdenum disulfide powder (<2 μm, 98%) and N, N-dimethylformamide (DMF) were purchased from Sigma Aldrich.

All reagents and chemicals used in this study were of analytical grade and were used without further purification.

Synthesis of Cs_xWO₃ Nanorods

Tungsten hexachloride (0.2976 g) was added to anhydrous ethanol (40 ml) under intense stirring, resulting in the formation of a yellowish solution. Thereafter, 0.065 g of CsOH·H₂O was introduced into the yellowish solution. After the resultant solution became homogeneous, 10 ml of acetic acid was added. Subsequently, the mixture was transferred into a 100 ml Teflon-lined autoclave, followed by hydrothermal treatment at 240°C for 20 h. Afterward, it was cooled to room temperature naturally, and the blue product was centrifuged, washed with ethanol several times, and finally dried in a vacuum oven at 60°C for 8 h (Wu et al., 2021).

Exfoliation of MoS₂ Nanosheets

The MoS₂ nanosheets were exfoliated by ultrasonication according to a previously reported method (Bera and sciences, 2017). Bulk MoS₂ (0.64 g) was added to DMF (20 ml) in a flat-bottomed beaker (100 ml) and ultrasonicated for 60 min. The temperature of the sonication was controlled by a cooling system during ultrasonication. Afterward, the sample was centrifuged, washed, and dried at 60°C for 8 h.

Preparation of Cs_xWO₃/MoS₂ Nanocomposites

The Cs_xWO₃/MoS₂ nanocomposite was prepared using a hydrothermal method. The material required for the synthesis—0.1 M aqueous solution of MoS₂ (30 ml) was stirred for 1 h. Simultaneously, 0.2976 g of tungsten hexachloride was mixed with 40 ml of anhydrous ethanol under intense stirring, which resulted in the formation of a yellowish solution. Thereafter, 0.065 g of CsOH·H₂O was added to the yellowish solution. Subsequently, 10 ml of acetic acid was added to the resultant solution when it became homogeneous. Afterward, different amounts of the prepared MoS₂ solution were added to form composites with different ratios. Subsequently, the mixture was transferred into a 100 ml Teflon-lined autoclave, followed by a hydrothermal process at 240°C for 20 h. The obtained dark blue product was centrifuged, washed with ethanol several times, and finally dried in a vacuum oven at 60°C. In this study, three different composites were prepared by changing the amount of MoS₂ and labeled as 5%, 15%, and 30%.

Characterization of Cs_xWO₃/MoS₂ Nanocomposites

Field emission scanning electron microscopy (FESEM, JSM6500F, JEOL, Tokyo, Japan), transmission electron microscopy (TEM), and high-resolution TEM (TEM, Philips-6500F) were used to study the surface morphologies of the samples. The crystal structures of the Cs_xWO₃, MoS₂, and Cs_xWO₃/MoS₂ nanocomposites were obtained by X-ray diffraction (XRD; D2 Phaser X-ray diffractometer, Bruker, Karlsruhe, Germany) analysis. The chemical compositions of the prepared samples were determined by Raman spectroscopy using an HR800 instrument (Jobin Yvon, Taipei, Taiwan). The N₂ adsorption/desorption isotherm and Brunauer, Emmett, and Teller (BET) surface area analyses of the samples were conducted at 77 K using a Quanta chrome iQ-MP gas adsorption analyzer (BEL JAPAN, INC.).

Sensor Fabrication and Hydrogen Gas Sensing Measurements

To fabricate the gas sensor, the as-prepared Cs_xWO₃, MoS₂, and Cs_xWO₃/MoS₂ nanocomposites were diluted with isopropanol (IPA) and spin-coated on Si/SiO₂ substrates, which were then sputtered with multi-finger Pt interdigitated electrodes (Figure 1). The H₂ gas sensing properties of the prepared sensors were measured in a compact vacuum chamber with an H₂ flow of 99.9% (diluted with dry air) via a mass flow controller. The properties were measured systematically from the electrical output response recorded using a Keithley source meter unit (SMU, Keithley 2,400, Tektronix, Beaverton, OR, USA) connected to a computer.

FIGURE 1

FIGURE 1. Schematic illustration of the synthesis process of Cs_xWO₃/MoS₂-based gas sensor.

Electrochemical Measurements of the Sensors

The electrochemical properties of the developed sensor materials were investigated by electrochemical impedance spectroscopy (EIS) using a 5,000 electrochemical workstation (Jiehan Technology Corp., Taiwan), wherein a conventional three-electrode configuration was used. In this measurement, 0.1 M aqueous solution of KCl was used as the electrolyte and platinum and Ag/AgCl were used as the counter and reference electrodes, respectively; a titanium substrate was used as the working electrode (Phuruangrat et al., 2009). To prepare the working electrode for EIS measurements, 4 mg of Cs_xWO₃, MoS₂, and 15% Cs_xWO₃/MoS₂ were added to 80 µL of Nafion solution and 920 µL of absolute ethanol, and the mixture was ultrasonicated for approximately 90 min to obtain a slurry. Thereafter, 40 µL of the slurry was drop-cast onto a 1 × 1 cm² titanium substrate electrode and dried at room temperature.

Results and Discussion

Morphological and Structural Properties of Cs_xWO₃/MoS₂ Nanocomposites

The surface morphologies of the prepared samples were studied by FESEM, and the FESEM image in Figure 2A shows that MoS₂ has a sheet-like morphology, mostly smaller than 2 µm in size. The FESEM image in Figure 2B depicts that the surface morphology of Cs_xWO₃ comprises a nanorod-like structure with an average diameter of 40–50 nm. The FESEM image of the 15% Cs_xWO₃/MoS₂ nanocomposite in Figure 2C shows the coexistence of nanorods and nanosheets, owing to surface morphologies of Cs_xWO₃ and MoS₂, confirming the successful synthesis of the intended nanocomposites. Furthermore, the corresponding EDS spectrum confirmed the existence of Mo and S from MoS₂; Cs, O, and W from Cs_xWO₃. The actual elemental composition of the 15% Cs_xWO₃/MoS₂ nanocomposite was also investigated and the result as shown in the inset of Figure 2D. It can be seen from the actual mass percentage and theoretical mass percentage of each element in the nanocomposites that they are almost the same. These results reveal that the Cs_xWO₃/MoS₂ nanocomposite was successfully prepared.

FIGURE 2

FIGURE 2. FESEM images of (A) MoS₂ nanosheets; (B) Cs_xWO₃ nanorods; (C) Cs_xWO₃/MoS₂ composites and (D) EDS Spectrum of 15% Cs_xWO₃/MoS₂ nanocomposites.

The FESEM image in Figure 3A and elemental mapping results of the 15% Cs_xWO₃/MoS₂ nanocomposites presented in Figures 3B–F show the homogeneous distribution of Mo, S, Cs, O, and W elements in the nanocomposite.

FIGURE 3

FIGURE 3. (A) FESEM image and elemental mapping of (B) Mo, (C) S, (D) Cs, (E) O, and (F) W of 15% Cs_xWO₃/MoS₂ nanocomposite.

The surface morphology of the synthesized 15% Cs_xWO₃/MoS₂ nanocomposite was further studied by TEM and HRTEM. The TEM image of 15% Cs_xWO₃/MoS₂ nanocomposite shown in Figure 4A can be ascribed to Cs_xWO₃ nanorods and MoS₂ nanosheets. The coexistence of the MoS₂ nanosheets and Cs_xWO₃ nanorods can be seen in the HRTEM image of the nanocomposite, as shown in Figure 4B. The lattice spacing of 0.32 nm corresponds to the (002) crystal plane of Cs_xWO₃ and that of 0.27 nm corresponds to the (100) crystal plane of MoS₂. The corresponding selected area electron diffraction (SAED) pattern in Figure 4C confirms the combination of both Cs_xWO₃ and MoS₂, where the dots forming the hexagonal shape are attributed to the MoS₂ nanosheets and those forming the triangle are ascribed to Cs_xWO₃ (Ahmadi et al., 2014). However, the SAED dots in Figure 4C form hexagonal and triangular shapes with minimal changes than those of individual Cs_xWO₃ and MoS₂. This can be attributed to the nanocomposite formation of Cs_xWO₃/MoS₂. These results confirm that the nanocomposite was successfully prepared, and the Cs_xWO₃ nanorods and MoS₂ nanosheets were in good contact, which would enhance the gas sensing property.

FIGURE 4

FIGURE 4. (A) TEM, (B) HRTEM, and (C) SAED pattern images of 15% Cs_xWO₃/MoS₂ nanocomposite.

Figure 5 shows the XRD patterns of the CxWO₃ nanorods, MoS₂ nanosheets, and their nanocomposites. The XRD pattern of the Cs_xWO₃ nanorods can be ascribed to the hexagonal phase of Cs_0.33WO₃ (JCPDS No. 83-1334) (Wu et al., 2021). The absence of additional diffraction peaks confirmed the successful synthesis of pure Cs_0.33WO₃. The XRD peaks of the MoS₂ nanosheets can be indexed to hexagonal phase of MoS₂ (JCPDS No. 65-1951) (Zhang et al., 2014). The XRD peaks of the Cs_xWO₃/MoS₂ nanocomposites comprise characteristic peaks of both Cs_xWO₃ and MoS₂, confirming the successful preparation of the nanocomposite. In addition, the peak intensity of Cs_xWO₃ at (200) diffraction peak decreases as the MoS₂ content increases. The crystallite size of the Cs_xWO₃ and MoS₂ in the synthesized 15% Cs_xWO₃/MoS₂ nanocomposite was determined by using the Scherrer equation as shown below:

$\mathit{D=}\frac{0.9\lambda }{\mathrm{\beta }\mathit{cos}\theta }(1)$

where $\lambda$ is the wavelength of X-ray used (0.154 nm), β is the full-width at the half maximum of the respective diffraction peak, and $\theta$ is the angle at the maximum peak (Bekena et al., 2019). The finding shows that the crystallite size of Cs_xWO₃ was 2 nm at diffraction peak of (200). While that of the MoS₂ nanocomposite is about 6 nm at (002) diffraction peak.

FIGURE 5

FIGURE 5. XRD results of pure Cs_xWO₃, pure MoS₂, and different ratios of Cs_xWO₃/MoS₂ nanocomposites.

The as-prepared samples were further characterized by Raman spectroscopy, and the Raman spectra are shown in Figure 6A. The spectra show that two major peaks were observed for the MoS₂ nanosheets, which be indexed to the 2H phase of MoS₂ and E_2g (308 cm⁻¹) and A_1g (408 cm⁻¹) activation modes (Vadivelmurugan et al., 2021). The E_2g mode corresponds to the plane vibration of S and Mo atoms, whereas the A_1g mode is attributed to the relative vibration of the S atom, which is in the plane direction (Yao et al., 2019). Further, the two weak peaks at 451 and 1599 cm⁻¹ indicate E_1g and the longitudinal acoustic phonon modes, respectively. In the case of Cs_xWO₃, the Raman peak at 731 cm⁻¹ corresponds to monoclinic Gama WO₃ and that at 935 cm⁻¹ corresponds to nanocrystalline Cs_xWO₃ (Okada et al., 2019). These peaks in Cs_xWO₃ confirm the nanocrystalline formation of WO₃ with cesium. The characteristic peaks of both MoS₂ and Cs_xWO₃ were observed for Cs_xWO₃/MoS₂ composite, indicating the successful preparation of the nanocomposites. In addition, there is a slight shift in the WO₃ peaks, at 872 and 993 cm⁻¹, which indicates the presence of different organizations of elemental WO₆ octahedral.

FIGURE 6

FIGURE 6. (A) Raman spectra and (B) N₂ adsorption-desorption isotherms of the pure Cs_xWO₃, pure MoS₂, and 15% Cs_xWO₃/MoS₂ nanocomposite.

The BET specific surface areas of the materials were investigated by N₂ adsorption analysis, and the results in Figure 6B show that all the samples exhibited N₂ adsorption-desorption isotherms similar to type IV curves according to the Brunauer-Deming-Deming-Teller classification (Wang et al., 2018). The specific surface areas of the pure Cs_xWO₃, pure MoS₂, and 15% Cs_xWO₃/MoS₂ nanocomposites were calculated from the linear region of the multipoint plot. The BET specific surface areas of Cs_xWO₃, MoS₂, and 15% Cs_xWO₃/MoS₂ nanocomposites were 31.1, 3.3, and 15.0 m²g⁻¹, respectively. Herein, the surface area of 15% Cs_xWO₃/MoS₂ was lower than that of pure Cs_xWO₃ because of the encompassing of the nanorods by the MoS₂ nanosheets. Compared to MoS₂ nanosheets, the 15% Cs_xWO₃/MoS₂ nanocomposites possessed a larger surface area, which is important for the adsorption of a higher amount of hydrogen gas, and would aid in enhancing the gas sensing properties of the sensor.

Hydrogen Gas Sensing Properties of Cs_xWO₃/MoS₂ Composites-Based Gas Sensors

The sensing properties of metal oxide-based gas sensors are usually measured in terms of their sensitivity and repeatability by varying the resistance values of gas and vacuum/air vs. time. The H₂ gas detection properties of the Cs_xWO₃/MoS₂ nanocomposites were tested at a gas concentration of 10–500 ppm at 25°C ( ∼ 35 RH %). The sensor response of the samples is calculated using Equation 2 for oxidizing gases and vice versa for reducing gases.

$S(\%)=\frac{R_g}{R_a}\times 100(2)$

where R is the resistance; a is the air atmosphere, and g is the gas atmosphere of the samples.

The gas-sensing performance of a sensor can be determined using the current-voltage (I-V) curve recorded before and after the adsorption of the gas. Herein, we also evaluated the H₂ gas sensing performance of 15% Cs_xWO₃/MoS₂ nanocomposites using I-V characteristics before and after the adsorption of hydrogen gas, and the results in Figure 7A show the change in the electrical performance in the presence of H₂ when compared with that of no hydrogen gas. Figure 7B shows the sensor response of the developed 15% Cs_xWO₃/MoS₂ nanocomposite gas sensor at different concentrations (500, 250, 100, and 10 ppm) of hydrogen gas. The developed sensor exhibited outstanding H₂ gas sensing properties with a 50.6% sensor response toward 500 ppm of H₂ gas with 60 and 120 s response and recovery time, respectively. These recovery time and response time are better than that of reported Pd/CNT/Ni H₂ gas sensor that has 312 s response time and 173 s recovery and Ni/Pd-graphene H₂ gas, which has 180 s response time and 720 s recover time. (Lin and Huang, 2012; Phan and Chung, 2014). This sensor response is superior to that of the H₂ gas sensor of pure Cs_xWO₃ (31.3%) (Wu et al., 2021), which indicates that nanocomposite formation has enhanced the sensitivity. Figure 7C presents the sensor response vs. concentration curve, which shows a linear increase in the sensor response with an increase in concentration, revealing that the developed sensor can be applied to detect a wide range of concentrations of H₂ gas. Figure 7D shows that the fabricated 15% Cs_xWO₃/MoS₂ nanocomposite H₂ gas sensor demonstrates excellent cyclic stability for the five consecutive cycles that are important for practical applications. These findings reveal the potential applicability of the developed 15% Cs_xWO₃/MoS₂ nanocomposite sensor for the detection of H₂ gas.

FIGURE 7

FIGURE 7. (A) I-V curves, (B) sensor response with respect to the H₂ gas concentration of 15% Cs_xWO₃/MoS₂-based hydrogen gas sensor, (C) variation of the sensing response of Cs_xWO₃ and 15% Cs_xWO₃/MoS₂-based hydrogen gas sensor at room temperature when exposed to different ppm hydrogen, and (D) repeatability of 15% Cs_xWO₃/MoS₂-based hydrogen gas sensor at 500 ppm.

Long-term stability of sensor is very important for practical application. Herein, the long-term stability of the developed sensor was investigated. The result as shown in Figure 8A shows that it has excellent long-term stability during the 11-days evaluation period. Moreover, selectivity of the fabricated 15% Cs_xWO₃/MoS₂ nanocomposite hydrogen gas sensor was also studied. The finding in Figure 8B indicates that the 15% Cs_xWO₃/MoS₂ nanocomposite sensor presented excellent selectivity towards hydrogen gas by showing only 4 and 5% sensor response toward ammonia and carbon dioxide, respectively. The sensor response of the developed sensor toward CO₂ and NH₃ is neglible when compared with that of H₂ (50.6%). These findings confirm that developed sensor has potential applicability for real application for H₂ gas sensing. The sensing property of the developed sensor with respect to current versus time was also investigated. As it can be seen in Supplementary Figure S1, the current response of the fabricated sensor increases with increasing H₂ gas concentration, which proves the behavior of the n-type semiconductor sensor (Wisitsoraat et al., 2009; Mohamad et al., 2010). Moreover, the pure Cs_xWO₃ and MoS₂ also have the same properties (Saravanan et al., 2019; Wu et al., 2021).

FIGURE 8

FIGURE 8. (A) long-term stability, and (B) selectivity of the 15% Cs_xWO₃/MoS₂-based hydrogen gas sensor.

Figure 9 shows the sensor response of Cs_xWO₃/MoS₂ nanocomposites against different amount of MoS₂ (5%, 15%, and 30%) added to Cs_xWO₃. The sensor response of the nanocomposite initially increased with an increase in the amount of MoS₂ up to 15% MoS₂ addition and then decreased till 30% MoS₂ addition. This could be because of the encompassing of CsxWO₃ nanorods by MoS₂ nanosheets with low surface areas, which influences the adsorption of H₂ gas and consequently the sensor response (Supplementary Figure S2). The photograph of the prepared samples dispersed in IPA shown in Supplementary Figure S3 also confirms that the intensity of the dark color of the nanocomposite increases with an increase in the concentration of MoS₂ nanosheets, which confirms the presence of the high amount of MoS₂ in 30% MoS₂. Therefore, 15% Cs_xWO₃/MoS₂ nanocomposite was selected for further studies.

FIGURE 9

FIGURE 9. Sensor response of the Cs_xWO₃/MoS₂ nanocomposite sensor with respect to amounts of MoS₂ added to Cs_xWO₃.

Possible Hydrogen Gas Sensing Mechanisms of Cs_xWO₃/MoS₂ Nanocomposites

Metal oxide-based gas sensors, which sense hydrogen gas, are usually explained based on the variation of the electron depletion layer (EDL) and oxygen adsorption (Sun et al., 2011; Park et al., 2015; Wang et al., 2018). Herein, we propose a sensing mechanism for the developed sensor based on EDL. Cs_xWO₃ has oxygen defects in its structure, and MoS₂ is tuned to have a high bandgap after the exfoliation of bulk MoS₂. Therefore, the Cs_xWO₃ nanorods in the nanocomposite can adsorb oxygen from the air because of its oxygen vacancies, and the adsorbed oxygen extracts electrons from the conduction band and generates oxygen species and increases the width of the EDL (Figure 10A). In contrast, when the sensor is exposed to H₂ gas, the adsorbed oxygen species react with H₂ gas and produce extra electrons in the conduction band of CsxWO₃, which increase the electrical performance of the material and consequently the sensing property (Figure 10B).

FIGURE 10

FIGURE 10. Schematic illustration of Cs_xWO₃/MoS₂-based gas sensor (A) in air, and (B) in H₂ gas.

Further, the electrochemical properties of the samples were investigated, and the results in Figure 11 show that the EIS semicircle radius of the 15% Cs_xWO₃/MoS₂ nanocomposite is lower than those of pure Cs_xWO₃ and pure MoS₂, confirming that the nanocomposite has a higher electrical conductivity than those of pure materials, which contributed to the enhancement in the hydrogen gas sensor response.

FIGURE 11

FIGURE 11. Electrochemical impedance spectra of Cs_xWO₃, MoS₂, and 15% Cs_xWO₃/MoS₂.

The hydrogen gas sensing response of the developed 15% Cs_xWO₃/MoS₂ nanocomposite was also compared with those of reported hydrogen gas sensors, and the results in Table 1 indicate that the 15% Cs_xWO₃/MoS₂ nanocomposite exhibited a higher sensor response than those of other sensors (Esfandiar et al., 2012; Huang and Lin, 2012; Anand et al., 2014; Liu et al., 2015; Yang et al., 2015; Zhang et al., 2018; Sharma and Kim, 2018; Xiao et al., 2018; Wu et al., 2021). Further, some of the reported sensors can only operate at high temperatures. Therefore, the developed 15% Cs_xWO₃/MoS₂ nanocomposite H₂ gas sensor is a promising candidate for practical application in the detection of hydrogen gas.

TABLE 1

TABLE 1. Comparison of H₂ sensing properties of different metal oxide-based gas sensors.

Conclusion

In this study, Cs_xWO₃/MoS₂ nanocomposites were successfully prepared using the solvothermal method. The developed Cs_xWO₃/MoS₂ nanocomposite-based sensor exhibited outstanding hydrogen gas sensing properties with 51% response to 500 ppm H₂ gas. It also exhibits excellent cyclic stability. Further, the developed 15% Cs_xWO₃/MoS₂ nanocomposite demonstrated a superior H₂ gas sensing response at room temperature compared to reported H₂ gas sensors. The enhanced sensing response could be because of the improved electrical properties of the 15% Cs_xWO₃/MoS₂ nanocomposite. Therefore, this study facilitates the development of an effective and efficient H₂ gas sensor at room temperature, which will play a crucial role in the detection of hydrogen gas in the environment.

Data Availability Statement

The original contributions presented in the study are included in the article/Supplementary Material, further inquiries can be directed to the corresponding author.

Author Contributions

C-MW: Supervision, conceptualization and reviewing and editing. Shrisha: Methodology, data curation and writing. KM: Review and editing. G-YC: Methodology and data curation. D-HK: Resources. NG: Methodology.

Conflict of Interest

The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Publisher’s Note

All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors and the reviewers. Any product that may be evaluated in this article, orclaim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.

Acknowledgments

We would like to acknowledge the Ministry of Science and Technology of Taiwan, ROC for financially supporting part of this work, under contract numbers: MOST 110-2622-E-011-023.

Supplementary Material

The Supplementary Material for this article can be found online at: https://www.frontiersin.org/articles/10.3389/fmats.2022.831725/full#supplementary-material

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