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. 2025 Jun 5;15(11):871.
doi: 10.3390/nano15110871.

Excellent Room-Temperature NO2 Gas-Sensing Properties of TiO2-SnO2 Composite Thin Films Under Light Activation

Affiliations

Excellent Room-Temperature NO2 Gas-Sensing Properties of TiO2-SnO2 Composite Thin Films Under Light Activation

Victor V Petrov et al. Nanomaterials (Basel). .

Abstract

Thin TiO2-SnO2 nanocomposite films with high gas sensitivity to NO2 were synthesized by oxidative pyrolysis and comprehensively studied. The composite structure and quantitative composition of the obtained film nanomaterials have been confirmed by X-ray photoelectron spectroscopy, high-resolution transmission electron microscopy, and energy dispersive X-ray spectroscopy, which causes the presence of n-n heterojunctions and provides improved gas-sensitive properties. The sensor based on the 3TiO2-97SnO2 film has the maximum responses, which is explained by the existence of a strong surface electric field formed by large surface potentials in the region of TiO2-SnO2 heterojunctions detected by the Kelvin probe force microscopy method. Exposure to low-intensity radiation (no higher than 0.2 mW/cm2, radiation wavelength-400 nm) leads to a 30% increase in the sensor response relative to 7.7 ppm NO2 at an operating temperature of 200 °C and a humidity of 60% RH. At room temperature (20 °C), under humidity conditions, the response is 1.8 when exposed to 0.2 ppm NO2 and 85 when exposed to 7.7 ppm. The lower sensitivity limit is 0.2 ppm NO2. The temporal stability of the proposed sensors has been experimentally confirmed.

Keywords: SnO2; TiO2; composites; gas sensors; light activation; metal oxide; thin films.

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Conflict of interest statement

The authors declare no conflicts of interest.

Figures

Figure 1
Figure 1
Profilometry of a 3TiO2–97SnO2 film on a sensor platform.
Figure 2
Figure 2
TEM images of 1TiO2–99SnO2 with different scale (ac) and EDX analysis (df).
Figure 3
Figure 3
XPS spectra of TiO2–SnO2 films (a), high-resolution XPS spectrum Sn3d5 (b), O 1s (ce), Ti 2p (fh), for 1TiO2–99SnO2 (c,f), 3TiO2–97SnO2 (d,g), 5TiO2–95SnO2 (e,h). (ch) Red line—raw data; green—background; orange—fitted components (explanations are given in the text); blue line—envelope.
Figure 4
Figure 4
Dependence: (a) the roughness parameters Sq (curve 1) and Sy (curve 2); (b) the maximum values of the surface potential difference from the titanium ions concentration in the film.
Figure 5
Figure 5
Dependence of the conductivity logarithm of 1TiO2–99SnO2 (1), 3TiO2–97SnO2 (2), and 5TiO2–95SnO2 (3) films on the reverse temperature.
Figure 6
Figure 6
Optical transmission spectra (a) and band gap estimation for 1TiO2–99SnO2 (b), 3TiO2–97SnO2 (c), and 5TiO2–95SnO2 thin films (d).
Figure 7
Figure 7
Kinetics of the resistance change (ad) and temperature-dependence of the sensor response (e) based on the 1TiO2–99SnO2 film at a temperature of 100 °C and exposure to 7.7 ppm NO2 (curve 1) and under light activation ((b,d) and (e), curves 2 and 4), under the influence of 60% RH ((c,d) and (e), curves 3 and 4).
Figure 8
Figure 8
Kinetics of the resistance change (ad) and temperature-dependence of the sensor response (e) based on the 3TiO2–97SnO2 film at a temperature of 100 °C and exposure to 7.7 ppm NO2 (curve 1) and under light activation ((b,d) and (e), curves 2 and 4), under the influence of 60% RH ((c,d) and (e), curves 3 and 4).
Figure 9
Figure 9
Kinetics of the resistance change (ac) and temperature-dependence of the sensor response (d) based on the 5TiO2–95SnO2 film at a temperature of 100 °C and exposure to 7.7 ppm NO2 (curve 1) and under light activation ((b,c) and (d), curves 2 and 4), under the influence of 60% RH ((c) and (d), curves 3 and 4).
Figure 10
Figure 10
Temperature-dependence of the sensors’ response for 1TiO2–99SnO2, 3TiO2–97SnO2, and 5TiO2–95SnO2 to an exposure of 7.7 ppm NO2: (a) without influence; (b) under light activation; (c) at 60% RH, (d) at 60% RH and under light activation. The operating temperature is 100 °C.
Figure 11
Figure 11
Concentration-dependence of the 1TiO2–99SnO2 sensor response to NO2 without exposure (a) and when exposed to light activation (b,d); at 60% RH (c,d).
Figure 12
Figure 12
Concentration-dependence of the 3TiO2–97SnO2 sensor response to NO2 without exposure (a) and when exposed to light activation (b,d); at 60% RH (c,d).
Figure 13
Figure 13
Concentration-dependence of the 5TiO2–95SnO2 sensor response to NO2 without exposure (a) and when exposed to light activation (b,d); at 60% RH (c,d).
Figure 14
Figure 14
3TiO2–97SnO2 sensors’ temporal stability when exposed to 3.85 ppm NO2 (RT) under light activation (a) and under light activation and 60% RH (b) on different days.

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