Enhanced Gas Sensing Performance of ZnO/Ti3C2Tx MXene Nanocomposite

A representative of titanium carbide MXene, Ti3C2Tx is a promising candidate for high performance gas sensing and has attracted significant attention. However, MXene naturally has a multilayer structure with low porosity, which prevents its gas-sensing activity. Zinc oxide (ZnO) has long been utilized as a gas detector. Despite its good response to multiple gases, high operation temperature has limited its widespread use as a gas-sensing material. In this study, a room-temperature toxic gas sensor was prepared from ZnO/Ti3C2Tx MXene nanocomposite consisting of 2D few-layered MXene and 1D ZnO nanoparticles. A simple technique for synthesizing the nanocomposite was established. The physicochemical properties of the nanocomposite were fine-controlled with more active sites and higher porosity. The sensitivity and gas-selectivity of the sensing material were closely examined. The nanocomposite showed enhanced response and recovery behaviors to toxic gases, which outperformed pure Ti3C2Tx MXene and pure ZnO. This study offers a practical strategy by which to increase the gas-sensing performance of Ti3C2Tx MXene, and expands comprehensive understanding of the gas-sensing process of ZnO/Ti3C2Tx p-n heterostructure.


Introduction
MXenes, also known as two-dimensional (2D) carbides, nitrides, and carbonitrides, have gained huge attention due to their unique surface properties, morphology, and potential applications [1][2][3]. MXenes are represented by the general formula: M n+1 X n T x (n = 1-4), where M stands for transition metals, X stands for carbon or nitrogen, and T x holds for a functional group such as fluorine, hydroxyl, and oxygen [4][5][6]. Mostly, MXenes have been researched for gas sensing due to the ease of tuning the surface termination groups. Among various MXenes, titanium carbide (Ti 3 C 2 T x MXene) has been studied the most, due to its high electron density and sensitive interactions with toxic gas molecules [2,7,8].
However, while MXenes have been proven to be useful, their poor stability in humid environments and loss in surface area after hydration limit its potential applications [9][10][11]. In addition, low-porosity and high operating temperatures have caused various complications during their synthesis process [12,13]. This is why there is a need for the incorporation of other materials in combination with pure MXenes.
Some efforts have been made by scientists to sensitize Ti 3 C 2 T x MXene [14][15][16][17]. In our previous study, we synthesized Si-doped TiO 2 /Ti 3 C 2 T x hybridstructure using a diffusion process of Si atom at 1000 • C for enhancing NO 2 sensing activity [18]. Zhao et al. explored PANI/Ti 3 C 2 T x nanocomposite to enhance ethanol sensing properties [19]. In 2021, Yang et al. studied crumpled ZnO/Ti 3 C 2 T x sphere, using ultrasonic spray pyrolysis technique to improve the NO 2 sensing performance [20]. In fact, in these previous works, a certain unilateral parameter of the sensor was enhanced. The comprehensive sensing activity of the response and recovery values should therefore be further improved [21,22]. In this work, we have highlighted the enhanced gas sensing performance of ZnO/Ti 3 C 2 T x MXene nanocomposite at room-temperature. To increase the surface area of the material, we incorporated 1D ZnO nanoparticles on the surface of 2D few-layered MXene. The ZnO/Ti 3 C 2 T x MXene nanocomposite significantly improved the performance for toxic gas sensing. In addition, it was found that the response and recovery time of the ZnO/Ti 3 C 2 T x MXene nanocomposite outperformed the pure ZnO NPs and Ti 3 C 2 T x MXene. Furthermore, the gas-sensing process of ZnO/Ti 3 C 2 T x p-n heterostructure revealed better stability and performance than Ti 3 C 2 T x MXene in gas sensing.

Preparation of Ti 3 C 2 T x MXene and ZnO/Ti 3 C 2 T x Nanocomposites
First, multilayered Ti 3 C 2 T x MXenes were prepared by selectively etching Al layers from the pristine Ti 3 AlC 2 powder. Typically, a 2.0 g of pristine Ti 3 AlC 2 MAX phase was gradually immersed into 56 mL of a concentrated HF under continuous stirring at 300 rpm in an ice bath to avoid heat generation, and the mixed solution was transferred to an oil bath at 50 • C [23,24]. After one day of reaction, the MXene multilayer structures were collected and washed several times with DI water. Subsequently, a sample of few-layered Ti 3 C 2 T x MXene was prepared by ultrasonic probe sonicator (Sonics & Materials INC, Newtown, CT, USA) for around 30 min using multilayered MXene. Then, the obtained precipitate was dried overnight using a freeze-drying system (ilShinBioBase Co. Ltd., Gyeonggi-do, Korea) for further experiments.
ZnO/Ti 3 C 2 T x nanocomposites were synthesized by a simple technique, as schematically shown in Figure 1. Briefly, varying amounts (100, 200, and 300 mg) of the few-layered Ti 3 C 2 T x MXene powders were added to 25 mL of Zn 2+ solution. A total of 340 mg of KOH was dispersed in 15 mL of methanol under heat [25]. Subsequently, the two solutions were mixed to give the final precursor solution, which was kept under heat and sonication to form ZnO nanoparticles. After 30 min of reaction, the obtained products were continuously washed to remove the byproducts and named following real ratio as ZT1 (163:100), ZT2 (163:200), and ZT3 (163:300), respectively. Moreover, the pure ZnO nanoparticles were prepared for comparison in the same parameters without any Ti 3 C 2 T x MXene.
Micromachines 2022, 13, 1710 2 of improve the NO2 sensing performance [20]. In fact, in these previous works, a certain u lateral parameter of the sensor was enhanced. The comprehensive sensing activity of response and recovery values should therefore be further improved [21,22]. In this work, we have highlighted the enhanced gas sensing performance ZnO/Ti3C2Tx MXene nanocomposite at room-temperature. To increase the surface area the material, we incorporated 1D ZnO nanoparticles on the surface of 2D few-layer MXene. The ZnO/Ti3C2Tx MXene nanocomposite significantly improved the performan for toxic gas sensing. In addition, it was found that the response and recovery time of ZnO/Ti3C2Tx MXene nanocomposite outperformed the pure ZnO NPs and Ti3C2Tx MXe Furthermore, the gas-sensing process of ZnO/Ti3C2Tx p-n heterostructure revealed bet stability and performance than Ti3C2Tx MXene in gas sensing.

Preparation of Ti3C2Tx MXene and ZnO/Ti3C2Tx Nanocomposites
First, multilayered Ti3C2Tx MXenes were prepared by selectively etching Al lay from the pristine Ti3AlC2 powder. Typically, a 2.0 g of pristine Ti3AlC2 MAX phase w gradually immersed into 56 mL of a concentrated HF under continuous stirring at 3 rpm in an ice bath to avoid heat generation, and the mixed solution was transferred to oil bath at 50 °C [23,24]. After one day of reaction, the MXene multilayer structures w collected and washed several times with DI water. Subsequently, a sample of few-layer Ti3C2Tx MXene was prepared by ultrasonic probe sonicator (Sonics & Materials INC, Ne town, CT, USA) for around 30 min using multilayered MXene. Then, the obtained prec itate was dried overnight using a freeze-drying system (ilShinBioBase Co. Ltd., Gyeong do, Korea) for further experiments.
ZnO/Ti3C2Tx nanocomposites were synthesized by a simple technique, as schema cally shown in Figure 1. Briefly, varying amounts (100, 200, and 300 mg) of the few-layer Ti3C2Tx MXene powders were added to 25 mL of Zn 2+ solution. A total of 340 mg of KO was dispersed in 15 mL of methanol under heat [25]. Subsequently, the two solutions w mixed to give the final precursor solution, which was kept under heat and sonication form ZnO nanoparticles. After 30 min of reaction, the obtained products were contin ously washed to remove the byproducts and named following real ratio as ZT1 (163:10 ZT2 (163:200), and ZT3 (163:300), respectively. Moreover, the pure ZnO nanopartic were prepared for comparison in the same parameters without any Ti3C2Tx MXene.

Characterizations and Gas Sensing Measurements
The X-ray diffraction (XRD) patterns of as-prepared samples were obtained using a high resolution X-ray diffractometer (Rigaku, SmartLab, Tokyo, Japan) equipped with 3 kW Cu Kα radiation. The morphology of all samples was collected using scanning electron microscopy (FESEM, Hitachi, S-4700, Tokyo, Japan) and high resolution transmission electron microscopy (HR-TEM, Tecnai, Hillsboro, OR, USA). The bonding states and surface characteristics of selected samples were analyzed by X-ray photoelectron spectroscopy (XPS, K α plus, Thermo Fisher Scientific, Waltham, MA, USA). The Brunauer-Emmett-Teller (BET) analysis was measured using a nitrogen adsorption-desorption system (Micromeritics, ASAP 2020, Norcross, GA, USA).
To achieve gas sensing properties, concentrated suspensions of the as-prepared samples were covered on a glass substrate (10 × 10 mm). The gas sensing measurements were measured in a stainless-steel chamber (682 cm 3 ) at room temperature. The real-time resistance of the samples, when exposed to the toxic target gas (R g ) and synthetic air (R a ), was measured through Au wires using a digital source measure unit (SMU, Keithley 2450) [26]. Five target gases (CO 2 , H 2 , CH 4 , NH 3 , and NO 2 ) were used as the tested gases at high and low humidity ambient. The different gas concentrations of the toxic gas were produced by mixing it with synthetic air using a flow and pressure controller (GMC 1200). The gas sensor response value of the nanocomposite was expressed using the following equation [27]:

Microstructures and Structural Components
Observation of morphological surfaces of the Ti 3 AlC 2 MAX phase, Ti 3 C 2 T x MXene, pure ZnO nanoparticles, and ZnO/Ti 3 C 2 T x nanocomposite were analyzed using FESEM with high-and low-magnification (FESEM, Hitachi, S-4700, Tokyo, Japan). As displayed in Figure 2a, the pristine MAX phase has terraced microstructures with an average grain below 8 µm. After etching the MAX phase in concentrated HF solution, the micromorphology of multilayered Ti 3 C 2 T x MXene accounts for an accordion-like sandwich, which exhibited successful Al-selective etching (Figure 2b). After sonicating the MXene multilayer for 30 min, a few-layered Ti 3 C 2 T x MXene were regularly obtained. It can be observed from the inset magnified image in Figure 2c that the thickness of the Ti 3 C 2 T x MXene was around 150-350 nm, which could be due to the few-layered Ti 3 C 2 T x MXene. The as-synthesized ZnO displayed a particle shape with a diameter of 60-100 nm, as shown in Figure 2d. Compared to the pure ZnO nanoparticles, the few-layered Ti 3 C 2 T x MXene might suppress the growth and accumulation of ZnO nanoparticles. The heterostructure could support, not only faster, but also excess diffusion paths for toxic target gases.
By focusing in further, the SEM image of ZnO/Ti 3 C 2 T x nanocomposite clearly showed that the ZnO exhibited particle morphology, and featured a side anchored freely on the MXene two sides, suggesting efficient assembly between few-layered Ti 3 C 2 T x MXene sheets and ZnO particles during the treatment process (Figure 2e,f). It was estimated that a single-layer Ti 3 C 2 T x flake (2 nm thick) and few-layer (2-5 nm thick) flakes. The SEM and elemental mapping measurements of ZnO/Ti 3 C 2 T x heterostructure (ZT2) suggested the presence of C, O, Ti, and Zn components in the nanocomposite. They displayed a highly homogeneous distribution of C, O, Ti, and Zn ( Figure 3a). Moreover, the EDX spectrum also exhibited obvious C, O, Ti, and Zn elements, which were valuable for the stability and performance of the nanocomposite. As presented in Figure 3b,c, the HR-TEM images demonstrated the modification between the two interfaces, where both Ti 3 C 2 T x MXenes and ZnO were cross-linked to each other. This local communication could enhance the interaction between electrons and gas molecules.     The XRD patterns of prepared samples are displayed in Figure 4a. Well-defined diffraction peaks can be seen at 2θ = 9.5 • , 19.1 • , 36.7 • , 38.7 • , 38.9 • , and 60.1 • , which are indexed to the planes (002), (004), (101), (104), (105), (110), respectively (JCPDS card No.52-0875) [16]. After the etching development, a remarkable peak (002) in pure Ti 3 C 2 T x MXene exhibits that Al was successfully corroded from the Ti 3 AlC 2 MAX phase. The chemical bonding between each layer was decreased by increasing the c parameter. Meanwhile, ZnO showed preferred growth in the (101) orientation in the nanocomposite, and prominent ZnO peaks were also observed at 2θ = 31.7 • and 34.4 • , which were indexed to (100) and (002) planes, respectively. These peaks corresponded with the pure ZnO and the wurtzite structure (JCPDS card No.36-1451) [28]. The absence of any TiO 2 peaks revealed that oxidation seemed to not occur in the combination procedure. Thus, the XRD results of synthesized samples were completely expected. As displayed in Figure 4b, both samples illustrated a type IV isotherm plot with a relative pressure from 0.42 to 1.0, indicating H3type hysteresis circles [29]. Moreover, the BET-specific surface area (SSA) of ZnO/Ti 3 C 2 T x was calculated to be 29.7 m 2 /g, which is a 3.9-fold increase compared with the SSA of the Ti 3 C 2 T x MXene (7.5 m 2 /g). The results evidenced that the SSA of ZnO/Ti 3 C 2 T x nanocomposite was significantly improved owing to ultra-sonication and decoration, which were expected to improve the active sites and enhance the transportation of electrons.
Micromachines 2022, 13,1710 The XRD patterns of prepared samples are displayed in Figure 4a. Well-def fraction peaks can be seen at 2θ = 9.5°, 19.1°, 36.7°, 38.7°, 38.9°, and 60.1°, whic dexed to the planes (002), (004), (101), (104), (105), (110), respectively (JCPDS car 0875) [16]. After the etching development, a remarkable peak (002) in pure Ti3C2T exhibits that Al was successfully corroded from the Ti3AlC2 MAX phase. The c bonding between each layer was decreased by increasing the c parameter. Me ZnO showed preferred growth in the (101) orientation in the nanocomposite, and nent ZnO peaks were also observed at 2θ = 31.7° and 34.4°, which were indexed and (002) planes, respectively. These peaks corresponded with the pure ZnO wurtzite structure (JCPDS card No.36-1451) [28]. The absence of any TiO2 peaks that oxidation seemed to not occur in the combination procedure. Thus, the XRD of synthesized samples were completely expected. As displayed in Figure 4b, bo ples illustrated a type IV isotherm plot with a relative pressure from 0.42 to 1.0, in H3-type hysteresis circles [29]. Moreover, the BET-specific surface area ( ZnO/Ti3C2Tx was calculated to be 29.7 m 2 /g, which is a 3.9-fold increase compa the SSA of the Ti3C2Tx MXene (7.5 m 2 /g). The results evidenced that the SSA of ZnO nanocomposite was significantly improved owing to ultra-sonication and de which were expected to improve the active sites and enhance the transportation trons.

Chemical Binding States
The surface chemical and binding energy of ZnO/Ti3C2Tx nanocomposite served in detail using XPS measurement for Ti 2p, C 1s, Zn 2p, and O 1s. The re displayed in Figure 5. The overall XPS survey spectrum of ZnO/Ti3C2Tx heterostr illustrated in Figure 5a, indicating the existence of Zn 2p, O 1s, Ti 2p, and C 1s. Me Figure 5b-e reveals the various focused XPS spectra of individual elements. Fi showing a Ti 2p XPS spectra, indicates peaks at 454.9, 458.8, and 461.08 eV, corres to Ti-C, Ti-C and Ti-O, which may originate from C-Ti 3+ -Tx and C-Ti 2+ -Tx with Tx O-, -F, respectively [30]. Figure 5c reveals the C 1s high-resolution spectrum, fitt two main components at 284.7 and 281.2 eV, which could originate from graph and C-Ti with a surface termination group, respectively [31]. Additionally, two m

Chemical Binding States
The surface chemical and binding energy of ZnO/Ti 3 C 2 T x nanocomposite was observed in detail using XPS measurement for Ti 2p, C 1s, Zn 2p, and O 1s. The results are displayed in Figure 5. The overall XPS survey spectrum of ZnO/Ti 3 C 2 T x heterostructure is illustrated in Figure 5a, indicating the existence of Zn 2p, O 1s, Ti 2p, and C 1s. Meanwhile, Figure 5b-e reveals the various focused XPS spectra of individual elements. Figure 5b, showing a Ti 2p XPS spectra, indicates peaks at 454.9, 458.8, and 461.08 eV, corresponding to Ti-C, Ti-C and Ti-O, which may originate from C-Ti 3+ -T x and C-Ti 2+ -T x with T x = -OH, -O-, -F, respectively [30]. Figure 5c reveals the C 1s high-resolution spectrum, fitted using two main components at 284.7 and 281.2 eV, which could originate from graphitic C=C, and C-Ti with a surface termination group, respectively [31]. Additionally, two main electronic states of Zn 2p, shown in Figure 5d, spotted at 1045.9 and 1023.0 eV by a spin separation of 22.9 eV, are assigned to Zn 2p 1/2 and Zn 2p 3/2 , respectively [20]. As shown in Figure 5e, the O 1s high-resolution spectrum of the nanocomposite exhibited that the two prominent binding energy peaks at 530.2 and 532.2 eV could be assigned to O-Ti and C-Ti-T x (T x = -OH), respectively [32]. Therefore, the above results could deduce that the optimized nanocomposite exhibited an enhanced gas sensing performance.
Micromachines 2022, 13, 1710 6 of 10 tronic states of Zn 2p, shown in Figure 5d, spotted at 1045.9 and 1023.0 eV by a spin separation of 22.9 eV, are assigned to Zn 2p1/2 and Zn 2p3/2, respectively [20]. As shown in Figure 5e, the O 1s high-resolution spectrum of the nanocomposite exhibited that the two prominent binding energy peaks at 530.2 and 532.2 eV could be assigned to O-Ti and C-Ti-Tx (Tx = -OH), respectively [32]. Therefore, the above results could deduce that the optimized nanocomposite exhibited an enhanced gas sensing performance.

Gas Sensing Performance and Sensing
In order to find the performance of the excellent gas-sensitive and selective activity of ZnO/Ti3C2Tx nanocomposite, the gas sensing activities of pure MXene, pure ZnO, and ZnO/Ti3C2Tx with different MXene weight ratios were also recorded and shown in Figure  6. Figure 6a,b illustrates the response of ZT1, ZT2, ZT3, and pure MXene sensors to NO2 concentrations at 5 ppm and 10 ppm, respectively. The response signal of pure ZnO did not detect at room temperature, indicating semiconductor characteristics. The response signals of all the sensors were enhanced with the increase of NO2 concentration, while the response of pure Ti3C2Tx MXene was not well developed with noise signals, due to metallic behavior. The responses to 5 and 10 ppm NO2 were calculated at 35 % and 54 %, respectively. The NO2 response and recovery properties of ZT2 at room temperature were more substantial than those of ZT1 and ZT3, which were inadequate (Figure 6b).
In addition, the saturation time of the ZnO/Ti3C2Tx heterostructure to NO2 was recorded. For this evaluation, the ZT2 sensor was exposed to NO2 at a time interval of 5 min. After 10 min, the sensing signal seemed to be saturated, as shown in Figure 6c. For further clarification, Figure 6d displays the sensing response to 10ppm of various gases (e.g., H2, NH3, CH4, NO2, CO2) based on the ZnO/Ti3C2Tx sensor. It can be observed that the ZT2 nanocomposite had the significant response to NO2 in comparison with other gases at low and high humidity.
In order to further explore the sensing activities of ZnO/Ti3C2Tx heterostructure to NO2 gas molecules, the ZT2 sensor was exposed to various NO2 concentrations ranging from 5 to 30 ppm. As illustrated in Figure 6e, the result increased with the rising concentration of NO2, exhibiting that the proposed ZT2 to NO2 molecule was logarithmic with the linear regression (R 2 ) of 0.992 was acquired. Moreover, the repeatable cycle to 5-30 ppm NO2 molecules of the ZT2 sensor, provided in Figure 6f, reveals that the sensor possesses a repeatable characteristic. The gas sensing performance of Ti3C2Tx-based sensors is summarized in Table 1. Although our ZnO/Ti3C2Tx sensor did not show a remarkable NO2

Gas Sensing Performance and Sensing
In order to find the performance of the excellent gas-sensitive and selective activity of ZnO/Ti 3 C 2 T x nanocomposite, the gas sensing activities of pure MXene, pure ZnO, and ZnO/Ti 3 C 2 T x with different MXene weight ratios were also recorded and shown in Figure 6. Figure 6a,b illustrates the response of ZT1, ZT2, ZT3, and pure MXene sensors to NO 2 concentrations at 5 ppm and 10 ppm, respectively. The response signal of pure ZnO did not detect at room temperature, indicating semiconductor characteristics. The response signals of all the sensors were enhanced with the increase of NO 2 concentration, while the response of pure Ti 3 C 2 T x MXene was not well developed with noise signals, due to metallic behavior. The responses to 5 and 10 ppm NO 2 were calculated at 35% and 54%, respectively. The NO 2 response and recovery properties of ZT2 at room temperature were more substantial than those of ZT1 and ZT3, which were inadequate (Figure 6b).
In addition, the saturation time of the ZnO/Ti 3 C 2 T x heterostructure to NO 2 was recorded. For this evaluation, the ZT2 sensor was exposed to NO 2 at a time interval of 5 min. After 10 min, the sensing signal seemed to be saturated, as shown in Figure 6c. For further clarification, Figure 6d displays the sensing response to 10ppm of various gases (e.g., H 2 , NH 3 , CH 4 , NO 2 , CO 2 ) based on the ZnO/Ti 3 C 2 T x sensor. It can be observed that the ZT2 nanocomposite had the significant response to NO 2 in comparison with other gases at low and high humidity.
In order to further explore the sensing activities of ZnO/Ti 3 C 2 T x heterostructure to NO 2 gas molecules, the ZT2 sensor was exposed to various NO 2 concentrations ranging from 5 to 30 ppm. As illustrated in Figure 6e, the result increased with the rising concentration of NO 2 , exhibiting that the proposed ZT2 to NO 2 molecule was logarithmic with the linear regression (R 2 ) of 0.992 was acquired. Moreover, the repeatable cycle to 5-30 ppm NO 2 molecules of the ZT2 sensor, provided in Figure 6f, reveals that the sensor possesses a repeatable characteristic. The gas sensing performance of Ti 3 C 2 T x -based sensors is summarized in Table 1. Although our ZnO/Ti 3 C 2 T x sensor did not show a remarkable NO 2 response compared with other sensors, it is a promising candidate for NO 2 detection at room temperature.

Conclusions
In summary, the preparation of ZnO/Ti3C2Tx MXene nanocomposite by effective ultrasonication was investigated. In comparison with pure ZnO nanoparticles and Ti3C2Tx MXene, the optimized nanocomposite achieved sensitivity and selectivity to NO2 gas sensing. The response to 5 ppm NO2 was calculated at 35% with a speedy recovery and long-term stability at room temperature. The high sensitivity NO2 sensing activity of ZnO/Ti3C2Tx MXene nanocomposite was ascribed to the active sites and defects, which were the p-n heterointerface contacts between ZnO nanoparticles and Ti3C2Tx MXene. The results of this combination structure pave the way for the chemical sensing of Ti3C2Tx MXene-based materials, thus providing a reference by which to understand the fundamentals of Ti3C2Tx MXene gas sensing.   During the checking of NO 2 sensing properties, it was expected that the NO 2 gas would react with O 2 − species to form NO 3 − species, owing to the oxygen having lower electronegativity than the target gas [20,36,37]. Simultaneously, NO 2 gas collected electrons and enhanced the depletion layer, thus improving the response and recovery values. Moreover, NO 2 gas can be absorbed on the surface of p-type Ti 3 C 2 T x MXene due to its oxidizing and electrophilic properties, resulting in reduced resistance [38]. Essentially, ZnO nanoparticles with an n-doping effect were decorated with a number of negative oxygen species (O 2 − ) on the surface and supported an important role in the absorption of NO 2 [39]. Under ambient humidity, the hydrogen bonding between NO 2 and H 2 O molecules further promoted the chemical adsorption of NO 2 [40]. The electron donation reaction can be described as follows [20,41,42]: O − (ads) + e − → O 2− (ads) NO 2 (g) → NO 2 (ads) (6) NO 2 (ads) + e − → NO 2 − (ads) 2NO 2 (ads) + O 2 − (ads) + 2e − → 2NO 3 − (ads) (8)

Conclusions
In summary, the preparation of ZnO/Ti 3 C 2 T x MXene nanocomposite by effective ultrasonication was investigated. In comparison with pure ZnO nanoparticles and Ti 3 C 2 T x MXene, the optimized nanocomposite achieved sensitivity and selectivity to NO 2 gas sensing. The response to 5 ppm NO 2 was calculated at 35% with a speedy recovery and long-term stability at room temperature. The high sensitivity NO 2 sensing activity of ZnO/Ti 3 C 2 T x MXene nanocomposite was ascribed to the active sites and defects, which were the p-n heterointerface contacts between ZnO nanoparticles and Ti 3 C 2 T x MXene. The results of this combination structure pave the way for the chemical sensing of Ti 3 C 2 T x MXene-based materials, thus providing a reference by which to understand the fundamentals of Ti 3 C 2 T x MXene gas sensing.