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Bidimensional Engineered Amorphous a-SnO(2) Interfaces: Synthesis and Gas Sensing Response to H(2)S and Humidity

[Image: see text] Two-dimensional (2D) transition metal dichalcogenides (TMDs) and metal chalcogenides (MCs), despite their excellent gas sensing properties, are subjected to spontaneous oxidation in ambient air, negatively affecting the sensor’s signal reproducibility in the long run. Taking advant...

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Autores principales: Paolucci, Valentina, De Santis, Jessica, Ricci, Vittorio, Lozzi, Luca, Giorgi, Giacomo, Cantalini, Carlo
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9315963/
https://www.ncbi.nlm.nih.gov/pubmed/35757893
http://dx.doi.org/10.1021/acssensors.2c00887
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author Paolucci, Valentina
De Santis, Jessica
Ricci, Vittorio
Lozzi, Luca
Giorgi, Giacomo
Cantalini, Carlo
author_facet Paolucci, Valentina
De Santis, Jessica
Ricci, Vittorio
Lozzi, Luca
Giorgi, Giacomo
Cantalini, Carlo
author_sort Paolucci, Valentina
collection PubMed
description [Image: see text] Two-dimensional (2D) transition metal dichalcogenides (TMDs) and metal chalcogenides (MCs), despite their excellent gas sensing properties, are subjected to spontaneous oxidation in ambient air, negatively affecting the sensor’s signal reproducibility in the long run. Taking advantage of spontaneous oxidation, we synthesized fully amorphous a-SnO(2) 2D flakes (≈30 nm thick) by annealing in air 2D SnSe(2) for two weeks at temperatures below the crystallization temperature of SnO(2) (T < 280 °C). These engineered a-SnO(2) interfaces, preserving all the precursor’s 2D surface-to-volume features, are stable in dry/wet air up to 250 °C, with excellent baseline and sensor’s signal reproducibility to H(2)S (400 ppb to 1.5 ppm) and humidity (10–80% relative humidity (RH)) at 100 °C for one year. Specifically, by combined density functional theory and ab initio molecular dynamics, we demonstrated that H(2)S and H(2)O compete by dissociative chemisorption over the same a-SnO(2) adsorption sites, disclosing the humidity cross-response to H(2)S sensing. Tests confirmed that humidity decreases the baseline resistance, hampers the H(2)S sensor’s signal (i.e., relative response (RR) = R(a)/R(g)), and increases the limit of detection (LOD). At 1 ppm, the H(2)S sensor’s signal decreases from an RR of 2.4 ± 0.1 at 0% RH to 1.9 ± 0.1 at 80% RH, while the LOD increases from 210 to 380 ppb. Utilizing a suitable thermal treatment, here, we report an amorphization procedure that can be easily extended to a large variety of TMDs and MCs, opening extraordinary applications for 2D layered amorphous metal oxide gas sensors.
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spelling pubmed-93159632022-07-27 Bidimensional Engineered Amorphous a-SnO(2) Interfaces: Synthesis and Gas Sensing Response to H(2)S and Humidity Paolucci, Valentina De Santis, Jessica Ricci, Vittorio Lozzi, Luca Giorgi, Giacomo Cantalini, Carlo ACS Sens [Image: see text] Two-dimensional (2D) transition metal dichalcogenides (TMDs) and metal chalcogenides (MCs), despite their excellent gas sensing properties, are subjected to spontaneous oxidation in ambient air, negatively affecting the sensor’s signal reproducibility in the long run. Taking advantage of spontaneous oxidation, we synthesized fully amorphous a-SnO(2) 2D flakes (≈30 nm thick) by annealing in air 2D SnSe(2) for two weeks at temperatures below the crystallization temperature of SnO(2) (T < 280 °C). These engineered a-SnO(2) interfaces, preserving all the precursor’s 2D surface-to-volume features, are stable in dry/wet air up to 250 °C, with excellent baseline and sensor’s signal reproducibility to H(2)S (400 ppb to 1.5 ppm) and humidity (10–80% relative humidity (RH)) at 100 °C for one year. Specifically, by combined density functional theory and ab initio molecular dynamics, we demonstrated that H(2)S and H(2)O compete by dissociative chemisorption over the same a-SnO(2) adsorption sites, disclosing the humidity cross-response to H(2)S sensing. Tests confirmed that humidity decreases the baseline resistance, hampers the H(2)S sensor’s signal (i.e., relative response (RR) = R(a)/R(g)), and increases the limit of detection (LOD). At 1 ppm, the H(2)S sensor’s signal decreases from an RR of 2.4 ± 0.1 at 0% RH to 1.9 ± 0.1 at 80% RH, while the LOD increases from 210 to 380 ppb. Utilizing a suitable thermal treatment, here, we report an amorphization procedure that can be easily extended to a large variety of TMDs and MCs, opening extraordinary applications for 2D layered amorphous metal oxide gas sensors. American Chemical Society 2022-06-25 2022-07-22 /pmc/articles/PMC9315963/ /pubmed/35757893 http://dx.doi.org/10.1021/acssensors.2c00887 Text en © 2022 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Paolucci, Valentina
De Santis, Jessica
Ricci, Vittorio
Lozzi, Luca
Giorgi, Giacomo
Cantalini, Carlo
Bidimensional Engineered Amorphous a-SnO(2) Interfaces: Synthesis and Gas Sensing Response to H(2)S and Humidity
title Bidimensional Engineered Amorphous a-SnO(2) Interfaces: Synthesis and Gas Sensing Response to H(2)S and Humidity
title_full Bidimensional Engineered Amorphous a-SnO(2) Interfaces: Synthesis and Gas Sensing Response to H(2)S and Humidity
title_fullStr Bidimensional Engineered Amorphous a-SnO(2) Interfaces: Synthesis and Gas Sensing Response to H(2)S and Humidity
title_full_unstemmed Bidimensional Engineered Amorphous a-SnO(2) Interfaces: Synthesis and Gas Sensing Response to H(2)S and Humidity
title_short Bidimensional Engineered Amorphous a-SnO(2) Interfaces: Synthesis and Gas Sensing Response to H(2)S and Humidity
title_sort bidimensional engineered amorphous a-sno(2) interfaces: synthesis and gas sensing response to h(2)s and humidity
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9315963/
https://www.ncbi.nlm.nih.gov/pubmed/35757893
http://dx.doi.org/10.1021/acssensors.2c00887
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