Eco-Friendly Disposable WS2 Paper Sensor for Sub-ppm NO2 Detection at Room Temperature

We developed inexpensive and disposable gas sensors with a low environmental footprint. This approach is based on a biodegradable substrate, paper, and features safe and nontoxic electronic materials. We show that abrasion-induced deposited WS2 nanoplatelets on paper can be employed as a successful sensing layer to develop high-sensitivity and selective sensors, which operate even at room temperature. Its performance is investigated, at room temperature, against NO2 exposure, finding that the electrical resistance of the device drops dramatically upon NO2 adsorption, decreasing by ~42% (~31% half a year later) for 0.8 ppm concentration, and establishing a detection limit around~2 ppb (~3 ppb half a year later). The sensor is highly selective towards NO2 gas with respect to the interferents NH3 and CO, whose responses were only 1.8% (obtained for 30 ppm) and 1.5% (obtained for 8 ppm), respectively. Interestingly, an improved response of the developed sensor under humid conditions was observed (tested for 25% relative humidity at 23 °C). The high-performance, in conjunction with its small dimensions, low cost, operation at room temperature, and the possibility of using it as a portable system, makes this sensor a promising candidate for continuous monitoring of NO2 on-site.


Introduction
Gas sensing is becoming more and more important in our society. In fact, detection of various gases in low concentrations is crucial (and sometimes even mandatory) in fields such as air quality assessment, greenhouse gas emissions control, the quantification of volatiles for smart maintenance in the industry sector, and identification of biomarkers in medical diagnosis [1][2][3][4][5].
Among the gaseous species that should be monitored, detection of nitrogen dioxide (NO 2 ) is required in different applications. In the atmosphere, NO 2 plays the role of greenhouse gas and causes acid rain and photochemical smog problems [6]. Long-term exposure to high levels of NO 2 produces harmful effects for humans and other living beings [7,8]. Additionally, nitrogen oxides (NO x ) in exhaled breath are biomarkers for inflammatory and oxidative changes in lungs, serving as early indicators of the pathophysiology of many respiratory diseases [9].
Chemical sensors based on semiconductor materials [10][11][12][13][14][15], and particularly metal oxides, are the most popular devices to sense NO 2 gas [16][17][18][19]. However, these metal-oxidebased devices present poor sensitivity at room temperature, requiring high-temperature operation that leads to high power consumption and the eventual degradation of the sensing material [20]. Moreover, metal-oxide devices require the use of substrates compatible with micro-fabrication techniques (i.e., silicon, glass, quartz, etc.), which hampers their application in disposable electronics applications where the use of ultra-low cost and biodegradable substrates is crucial to emerging technologies and environmental impacts.
Over the past two decades, thanks to the revival of interest in van der Waals materials aroused by the isolation of graphene [21], sensors based on layered materials have been presented as a real step forward in gas sensing. Their exceptionally large surface-area-tovolume ratio makes these materials strongly sensitive to adsorbed gases, and therefore they are promising candidates for gas detection [22][23][24][25][26][27][28]. In fact, over the last years, several examples of NO 2 gas sensors based on van der Waals materials, operating even at room temperature, have been proved [26,[29][30][31][32].
The attractive properties of the conventional printer paper as a substrate, mainly its environmental-friendliness and low-cost, have led researchers to develop paper-based devices for various applications, including memory devices [33], solar cells [34,35], RFIDenabled wireless sensors [36], or supercapacitors [37]. Recently, some of the authors have demonstrated the integration of van der Waals materials on paper substrates through direct abrasion against the rough surface of paper [38][39][40][41]. However, only light and temperature sensors have been demonstrated so far, with gas sensing remaining unexplored. Because of the combination of ultra-low cost, availability, and biodegradability of paper substrates, integrating van der Waals materials on paper substrates opens the door for low-cost and disposable [42][43][44][45][46][47][48][49][50] gas sensors.
Here, we demonstrate the fabrication of gas sensors on standard copy paper substrates using abrasion-induced deposited WS 2 films as a sensing material. This process is simple to implement and yields low-cost and environmentally-friendly devices. In fact, standard copy paper substrates are biodegradable, and the sensing film (WS 2 ) and electrodes (graphite) are safe, nontoxic materials that can be found as natural minerals on Earth's crust. The sensing performance of the WS 2 -based sensor under exposure to NO 2 gas, operating at room temperature, is examined. Furthermore, the selectivity relative to potential interfering gases (NH 3 and CO) is analyzed [51][52][53].

Materials
Standard (untreated) copy printer paper (80 g/m 2 ) was used as supporting substrates because of its low cost and availability. Tungsten disulfide (WS 2 ) from HAGEN automation Ltd. (Bedford, UK) (0.6 microns APS Ultra Grade Micronized) was used as gas sensing channel material. Among the different semiconducting transition metal dichalcogenides, we selected WS 2 as it yielded films with the lower electrical resistance facilitating the electrical read-out of the fabricated devices. Graphite pencil (Madrid, Spain) (4B, Faber Castell) was employed to pattern graphite-based electrical leads (it has~80% of graphite content [54]) to connect the WS 2 channel to the readout electronics.

Sensor Fabrication
The steps for the gas sensor fabrication are depicted in Figure 1. First, the outline of the sensitive layer channel and electrodes were printed on the paper substrate ( Figure 1a). Then, a stencil mask (made of Nitto SPV 224 tape) delimited the sensitive area ( Figure 1b). Micronized WS 2 powder was rubbed against the unmasked paper substrate with a cotton swab (Figure 1c). The depositing process mimics the action of drawing/writing with a pencil on paper, where the friction forces between the van der Waals materials and paper cleaves the van der Waals crystals, leading to a network of interconnected platelets. The powder was abraded until a continuous film was reached. Then, the excess powder and the stencil mask were removed (Figure 1d). In the last process step, graphite electrodes were deposited on top of the sensitive material by drawing directly with a high-graphite content Nanomaterials 2022, 12, 1213 3 of 12 pencil (Figure 1e). These electrodes were contacted with spring-loaded probes (pogo pins) integrated inside the test chamber. Figure 1f shows a picture of the final device.
Nanomaterials 2022, 12, x FOR PEER REVIEW 3 of 12 the stencil mask were removed (Figure 1d). In the last process step, graphite electrodes were deposited on top of the sensitive material by drawing directly with a high-graphite content pencil (Figure 1e). These electrodes were contacted with spring-loaded probes (pogo pins) integrated inside the test chamber. Figure 1f shows a picture of the final device.

Material Characterization
Scanning electron microscopy (SEM) and energy dispersive X-ray spectroscopy (EDX), using a FE-SEM, FEI Nova NANOSEM 230 (Hillsboro, OR, USA), were used to characterize the morphology and the composition of the WS2 films deposited on paper. An electron energy of 7 keV was employed for imaging and 14 keV for EDX spectroscopy.

Experimental Setup
The chemoresistive sensor was placed inside a 6.25 mL volume airtight chamber for its characterization in different reducing and oxidizing atmospheres. Airflow inside the chamber was set to 100 mL/min, switching between gas sample for 10 min (exposition time) and synthetic air for 20 min (purge time). Gas cylinders supplied target gases with appropriate concentrations and balanced with the carrier gas (synthetic air): NO2 (1 ppm), CO (10 ppm), and NH3 (50 ppm) (all of them from Nippon Gases). Then, the initial sample concentration was diluted with synthetic air by using a gas mixing unit (GMU, Ray IE, Cáceres, Spain)to obtain the required exposed concentration. For proper control of the relative humidity (RH) inside the chamber, a handheld thermohygrometer RS1364 was used. The temperature was kept at 23 °C during the tests, and the required RH was achieved with a third flow controller that regulates the synthetic air bubbling through deionized water ( Figure 2).

Material Characterization
Scanning electron microscopy (SEM) and energy dispersive X-ray spectroscopy (EDX), using a FE-SEM, FEI Nova NANOSEM 230 (Hillsboro, OR, USA), were used to characterize the morphology and the composition of the WS 2 films deposited on paper. An electron energy of 7 keV was employed for imaging and 14 keV for EDX spectroscopy.

Experimental Setup
The chemoresistive sensor was placed inside a 6.25 mL volume airtight chamber for its characterization in different reducing and oxidizing atmospheres. Airflow inside the chamber was set to 100 mL/min, switching between gas sample for 10 min (exposition time) and synthetic air for 20 min (purge time). Gas cylinders supplied target gases with appropriate concentrations and balanced with the carrier gas (synthetic air): NO 2 (1 ppm), CO (10 ppm), and NH 3 (50 ppm) (all of them from Nippon Gases). Then, the initial sample concentration was diluted with synthetic air by using a gas mixing unit (GMU, Ray IE, Cáceres, Spain)to obtain the required exposed concentration. For proper control of the relative humidity (RH) inside the chamber, a handheld thermohygrometer RS1364 was used. The temperature was kept at 23 • C during the tests, and the required RH was achieved with a third flow controller that regulates the synthetic air bubbling through deionized water ( Figure 2).
The sensor was kept at room temperature while variations of the resistance over time were recorded with a digital multimeter (Keithley 2001). The experiment control and real time data acquisition was implemented with a PC using an in-house custom-made software developed with LabVIEW. The response of the sensor was calculated with the following equation: where R is the electrical resistance for the sensor in the tested gas and R 0 is the resistance of the sensor in the air. The sensor was kept at room temperature while variations of the resistance over time were recorded with a digital multimeter (Keithley 2001). The experiment control and real time data acquisition was implemented with a PC using an in-house custom-made software developed with LabVIEW. The response of the sensor was calculated with the following equation: where is the electrical resistance for the sensor in the tested gas and is the resistance of the sensor in the air.  Figure 3b shows a SEM image of the porous microscopic structure of the WS2 film deposited onto the paper substrate, formed by interconnected crystalline WS2 platelets, ensuring a very large effective surface area of the device. During the abrasion process, the WS2 flakes are cleaved, reducing their lateral dimensions to 1-5 µm and their thickness to sub-50 nm. Figure 3c shows a low magnification SEM image of a WS2 film obtained after its deposition on the paper substrate. The bare paper has fibrous-like structures arising from the cellulose fibers. The abrasion-induced deposition method yielded a continuous film of packed WS2 platelets covering the fibers. The bare paper and WS2 film can be easily distinguished because of their different contrast under SEM inspection. Figure 3d shows a SEM image of the sensitive area/electrode interface where it can be observed a sizable change in contrast due to the difference in electrical conductivity between the WS2 film and the WS2 film covered with graphite. The chemical composition of the film was characterized by energy dispersive X-ray (EDX) spectroscopy. Apart from the prominent W and S peaks, expected from the WS2 film, the spectrum had peaks associated with the presence of C and O, arising from the paper substrate. The spectrum also showed a Ca peak, attributed to the presence of calcium carbonate, a filler usually added to paper pulp to achieve a brighter white color (Figure 3e).   Figure 3b shows a SEM image of the porous microscopic structure of the WS 2 film deposited onto the paper substrate, formed by interconnected crystalline WS 2 platelets, ensuring a very large effective surface area of the device. During the abrasion process, the WS 2 flakes are cleaved, reducing their lateral dimensions to 1-5 µm and their thickness to sub-50 nm. Figure 3c shows a low magnification SEM image of a WS 2 film obtained after its deposition on the paper substrate. The bare paper has fibrous-like structures arising from the cellulose fibers. The abrasion-induced deposition method yielded a continuous film of packed WS 2 platelets covering the fibers. The bare paper and WS 2 film can be easily distinguished because of their different contrast under SEM inspection. Figure 3d shows a SEM image of the sensitive area/electrode interface where it can be observed a sizable change in contrast due to the difference in electrical conductivity between the WS 2 film and the WS 2 film covered with graphite. The chemical composition of the film was characterized by energy dispersive X-ray (EDX) spectroscopy. Apart from the prominent W and S peaks, expected from the WS 2 film, the spectrum had peaks associated with the presence of C and O, arising from the paper substrate. The spectrum also showed a Ca peak, attributed to the presence of calcium carbonate, a filler usually added to paper pulp to achieve a brighter white color ( Figure 3e).

Electrical Characterization
A thorough characterization of the electrical properties of abrasion-induced deposited WS 2 films on copy paper can be found in Ref [41]. Briefly, the resistivity of the films, determined through current vs. voltage measurements in transfer length configuration, ranges from~360 Ω·m to~530 Ω·m and electric field effect measurements demonstrated the p-type character of the WS 2 film. Additionally, in the mentioned reference, 118 devices were developed to study the reproducibility, showing a low dispersion taking into account the nature of the films: a random network of interconnected platelets where percolation transport is expected.
The sensor was kept at air atmosphere, and after a few minutes, the calculated rootmean square (RMS) noise level was approximately 0.01% for the sensor. Thanks to the electrical continuity of the WS 2 film, the device operates with low noise that is a consequence of the dry deposition method, and a good adhesion between sensitive material and paper fibers.

Electrical Characterization
A thorough characterization of the electrical properties of abrasion-induced deposited WS2 films on copy paper can be found in Ref [41]. Briefly, the resistivity of the films, determined through current vs. voltage measurements in transfer length configuration, ranges from ~360 Ω·m to ~530 Ω·m and electric field effect measurements demonstrated the p-type character of the WS2 film. Additionally, in the mentioned reference, 118 devices were developed to study the reproducibility, showing a low dispersion taking into account the nature of the films: a random network of interconnected platelets where percolation transport is expected.
The sensor was kept at air atmosphere, and after a few minutes, the calculated rootmean square (RMS) noise level was approximately 0.01% for the sensor. Thanks to the electrical continuity of the WS2 film, the device operates with low noise that is a consequence of the dry deposition method, and a good adhesion between sensitive material and paper fibers.

Gas Sensor Characterization
To characterize the performance of this sensor, its sensitivity, and response time, we studied the changes in resistance upon cyclic exposition and purge processes with NO2 at various concentrations ranges (0.2 ppm-0.8 ppm, see Figure 4a). The gas sensing mechanism is attributed to the surface reactions between the p-type WS2 platelets and gas molecules. In the case of a p-type semiconductor in an oxidant environment (NO2), the con-

Gas Sensor Characterization
To characterize the performance of this sensor, its sensitivity, and response time, we studied the changes in resistance upon cyclic exposition and purge processes with NO 2 at various concentrations ranges (0.2 ppm-0.8 ppm, see Figure 4a). The gas sensing mechanism is attributed to the surface reactions between the p-type WS 2 platelets and gas molecules. In the case of a p-type semiconductor in an oxidant environment (NO 2 ), the concentration of electrons on the surface decreases (the number of holes increases) and, consequently, the resistance of the WS 2 film decreases (Figure 4a). The sensor device showed a fast recovery with a low baseline drift of 0.6% at 0.8 ppm of NO 2 . Therefore, an automatic baseline subtraction method based on linear correction for measurements before exposition and in the final of the purge time was implemented.
In most real-life applications, the target gas is in a complex environment surrounded by several gases at different concentrations, requiring sensors with high sensitivity and selectivity to discriminate and classify the target gas. Important interfering gases, in the above applications, are carbon monoxide (CO) and ammonia (NH 3 ) [55,56]. Therefore, gas sensors with negligible interference between reducing and oxidizing environments, i.e., a high absolute selectivity, are highly desirable to achieve a more reliable signal interpretation. To test the selectivity of the WS 2 on paper NO 2 sensor, we have subjected the device to cyclic exposition and purge processes with CO and NH 3 at various concentrations ranges (1.5 ppm-8 ppm for CO and 10 ppm-30 ppm for NH 3 , see Figure 4b,c). Upon exposure to CO and NH 3 , the resistance increases as expected for a p-type semiconductor, because the generated electrons recombine with holes. The gas test showed the sensor has a remarkably higher sensitivity towards NO 2 (42% resistance change at 0.8 ppm) than NH 3 and CO, whose responses were 1.8% (obtained at 30 ppm) and 1.5% (obtained at 8 ppm), respectively (see Figure 5a,b). This can be justified by the adsorption kinetics of gas molecules on the sensitive material. Additionally, the high sensitivity and selectivity to NO 2 is consistent with results of density functional theory calculation in Ref. [32]. Interestingly, this article explains that the chemically reactive edge sites of WS 2 served as highly favorable active sites for direct interaction with target NO 2 gas molecules. This is consistent with the fact that abrasion-induced is an effective method to generate numerous edge sites in deposited WS 2 nanoplatelets on paper, since the technique induces fracturing, tearing, and peeling off from substrates. Nanomaterials 2022, 12, x FOR PEER REVIEW 6 of 12 centration of electrons on the surface decreases (the number of holes increases) and, consequently, the resistance of the WS2 film decreases (Figure 4a). The sensor device showed a fast recovery with a low baseline drift of 0.6% at 0.8 ppm of NO2. Therefore, an automatic baseline subtraction method based on linear correction for measurements before exposition and in the final of the purge time was implemented. In most real-life applications, the target gas is in a complex environment surrounded by several gases at different concentrations, requiring sensors with high sensitivity and selectivity to discriminate and classify the target gas. Important interfering gases, in the above applications, are carbon monoxide (CO) and ammonia (NH3) [55,56]. Therefore, gas sensors with negligible interference between reducing and oxidizing environments, i.e., a high absolute selectivity, are highly desirable to achieve a more reliable signal interpretation. To test the selectivity of the WS2 on paper NO2 sensor, we have subjected the device to cyclic exposition and purge processes with CO and NH3 at various concentrations ranges (1.5 ppm-8 ppm for CO and 10 ppm-30 ppm for NH3, see Figure 4b,c). Upon exposure to CO and NH3, the resistance increases as expected for a p-type semiconductor, because the generated electrons recombine with holes. The gas test showed the sensor has Accordingly, the response speed of the device was studied. We determined the response time parameter τ 90 , defined as the time necessary to reach approximately 90% of the response when the sensor is subjected to an abrupt change in atmosphere. The τ 90 values obtained were NO 2 5.2 min at 0.8 ppm, NH 3 8.8 min at 30 ppm, and CO 9.6 min at 8 ppm (Figure 5c). In comparison, the paper-based sensor showed the shortest response time for NO 2 that nearly achieved the equilibrium. In contrast, CO and NH 3 responses had not yet approached an equilibrium, resulting in a high sensitivity NO 2 gas sensor with insignificant NH 3 /CO-interference. Therefore, this very high selectivity with respect to potential interfering gases of the sensor is highly advantageous to be used for gas sensing applications.
a remarkably higher sensitivity towards NO2 (42% resistance change at 0.8 ppm) than NH3 and CO, whose responses were 1.8% (obtained at 30 ppm) and 1.5% (obtained at 8 ppm), respectively (see Figure 5a,b). This can be justified by the adsorption kinetics of gas molecules on the sensitive material. Additionally, the high sensitivity and selectivity to NO2 is consistent with results of density functional theory calculation in Ref. [32]. Interestingly, this article explains that the chemically reactive edge sites of WS2 served as highly favorable active sites for direct interaction with target NO2 gas molecules. This is consistent with the fact that abrasion-induced is an effective method to generate numerous edge sites in deposited WS2 nanoplatelets on paper, since the technique induces fracturing, tearing, and peeling off from substrates. Accordingly, the response speed of the device was studied. We determined the response time parameter τ90, defined as the time necessary to reach approximately 90% of the response when the sensor is subjected to an abrupt change in atmosphere. The τ90 values obtained were NO2 5.2 min at 0.8 ppm, NH3 8.8 min at 30 ppm, and CO 9.6 min at 8 ppm (Figure 5c). In comparison, the paper-based sensor showed the shortest response time for NO2 that nearly achieved the equilibrium. In contrast, CO and NH3 responses had not yet approached an equilibrium, resulting in a high sensitivity NO2 gas sensor with insignificant NH3/CO-interference. Therefore, this very high selectivity with respect to potential interfering gases of the sensor is highly advantageous to be used for gas sensing applications.
The structural continuity of the micronized WS2 particles deposited by abrasion provides higher electrical conductivity toward a lower limit of detection (LOD) compared to sensors fabricated by other methods, such as drop-casting [26]. From the response for 0.8 ppm of NO2, a theoretically achievable LOD of around 2 ppb was calculated, which is equivalent to a signal-to-noise ratio (SNR) value of three.
In order to assess the stability of these devices upon environmental degradation, we performed a new set of measurements half a year after its fabrication (the sensor was stored under ambient conditions during that time). Thereafter, the response for 0.8 ppm of NO2 was slightly decreased to 31%, increasing the LOD around 3 ppb ( Figure 6). In particular, the decrease of the gas response is small between measurements for a half year interval, which demonstrates that the paper-based sensor has a slow degradation, maintaining a high response over time. The effect of relative humidity on the paper-based sensor was tested at 23 °C with 25% RH and it responded efficiently to humidity, obtaining a maximum response of 114% (Figure 7a). Cross-sensitivity measurements were carried out The structural continuity of the micronized WS 2 particles deposited by abrasion provides higher electrical conductivity toward a lower limit of detection (LOD) compared to sensors fabricated by other methods, such as drop-casting [26]. From the response for 0.8 ppm of NO 2 , a theoretically achievable LOD of around 2 ppb was calculated, which is equivalent to a signal-to-noise ratio (SNR) value of three.
In order to assess the stability of these devices upon environmental degradation, we performed a new set of measurements half a year after its fabrication (the sensor was stored under ambient conditions during that time). Thereafter, the response for 0.8 ppm of NO 2 was slightly decreased to 31%, increasing the LOD around 3 ppb ( Figure 6). In particular, the decrease of the gas response is small between measurements for a half year interval, which demonstrates that the paper-based sensor has a slow degradation, maintaining a high response over time. The effect of relative humidity on the paper-based sensor was tested at 23 • C with 25% RH and it responded efficiently to humidity, obtaining a maximum response of 114% (Figure 7a). Cross-sensitivity measurements were carried out to assess the influence of RH on the sensor response to NO 2 . Figure 7b illustrates the effect of 0.8 ppm of NO 2 detection in an environment with a RH of 25% with a sensor response of~44%.
The experimental responses of NO 2 over time and under humid conditions were compared for 0.8 ppm (Figure 8a1-a4). In the days following device manufacture, the sensor had a high response close to 42% with an operating resistance of~4 MΩ. Then, after half a year where the sensor was stored in ambient conditions, the resistance increased tõ 22 MΩ, decreasing the response to~31%, which was attributed to the effects of sensor poisoning by gases surrounding in ambient during the half a year period. However, a positive effect of humid conditions (25% RH at 23 • C) is that at the same gas concentration the sensor response increased to 44%, simultaneously the resistance scaled up~142 MΩ. The improved response to NO 2 with humidity can be justified by the intrinsic and induced dipole moments of the molecules and their intermolecular charge transfer [57]. Finally, there was a practically total regeneration of the sensor after humidity exposition was obtained for dry synthetic air, and the sensor showed a response of~30% for a resistance operation of~42 MΩ (Figure 8b,c). Therefore, the sensor performance is a huge benefit since it can work on a large range of tests for multidisciplinary applications carried out in humid conditions with sensitivity gain. Nanomaterials 2022, 12, x FOR PEER REVIEW to assess the influence of RH on the sensor response to NO2. Figure 7b illustrates th of 0.8 ppm of NO2 detection in an environment with a RH of 25% with a sensor re of ~44%.  The experimental responses of NO2 over time and under humid condition compared for 0.8 ppm (Figure 8a-d). In the days following device manufacture, the had a high response close to 42% with an operating resistance of ~4 MΩ. Then, af a year where the sensor was stored in ambient conditions, the resistance increased MΩ, decreasing the response to ~31%, which was attributed to the effects of sens soning by gases surrounding in ambient during the half a year period. However, tive effect of humid conditions (25% RH at 23 °C) is that at the same gas concentrat to assess the influence of RH on the sensor response to NO2. Figure 7b illustrates t of 0.8 ppm of NO2 detection in an environment with a RH of 25% with a sensor r of ~44%.  The experimental responses of NO2 over time and under humid conditio compared for 0.8 ppm (Figure 8a-d). In the days following device manufacture, th had a high response close to 42% with an operating resistance of ~4 MΩ. Then, a a year where the sensor was stored in ambient conditions, the resistance increase MΩ, decreasing the response to ~31%, which was attributed to the effects of sen soning by gases surrounding in ambient during the half a year period. However tive effect of humid conditions (25% RH at 23 °C) is that at the same gas concentra sensor response increased to 44%, simultaneously the resistance scaled up ~142 M improved response to NO2 with humidity can be justified by the intrinsic and The improved response to NO2 with humidity can be justified by the intrinsic and induced dipole moments of the molecules and their intermolecular charge transfer [57]. Finally, there was a practically total regeneration of the sensor after humidity exposition was obtained for dry synthetic air, and the sensor showed a response of ~30% for a resistance operation of ~42 MΩ (Figure 8b,c). Therefore, the sensor performance is a huge benefit since it can work on a large range of tests for multidisciplinary applications carried out in humid conditions with sensitivity gain.

Conclusions
In summary, we fabricated and characterized a disposable NO2 sensor based on a ptype WS2 film on standard paper. The sensing film was deposited by a low-cost and easy to implement abrasion-induced method, establishing a nanostructured sensitive layer by exfoliation of micronized WS2 particles and an electrical connection among flakes. The structure of the WS2 sensing film was characterized by using SEM, which showed rough and porous film formed by interconnected WS2 flakes. The sensor showed excellent sensing properties at room temperature with a response higher than 42% (31% half a year later) at 0.8 ppm NO2 and with a significant LOD of around 2 ppb (3 ppb half a year later). The relative humidity of 25% at 23 °C has a beneficial impact. The result indicates the high sensitivity, selectivity, and repeatability of the presented sensor towards sub-ppm level of NO2 gas, which makes it a promising candidate for monitoring of NO2 sensing.

Conclusions
In summary, we fabricated and characterized a disposable NO 2 sensor based on a p-type WS 2 film on standard paper. The sensing film was deposited by a low-cost and easy to implement abrasion-induced method, establishing a nanostructured sensitive layer by exfoliation of micronized WS 2 particles and an electrical connection among flakes. The structure of the WS 2 sensing film was characterized by using SEM, which showed rough and porous film formed by interconnected WS 2 flakes. The sensor showed excellent sensing properties at room temperature with a response higher than 42% (31% half a year later) at 0.8 ppm NO 2 and with a significant LOD of around 2 ppb (3 ppb half a year later). The relative humidity of 25% at 23 • C has a beneficial impact. The result indicates the high sensitivity, selectivity, and repeatability of the presented sensor towards sub-ppm level of NO 2 gas, which makes it a promising candidate for monitoring of NO 2 sensing.