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Berholts A, Kodu M, Rubin P, Kahro T, Alles H, Jaaniso R. Layered Heterostructure of Graphene and TiO 2 as a Highly Sensitive and Stable Photoassisted NO 2 Sensor. ACS APPLIED MATERIALS & INTERFACES 2024; 16:43827-43837. [PMID: 39110038 PMCID: PMC11345727 DOI: 10.1021/acsami.4c08151] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/17/2024] [Revised: 07/25/2024] [Accepted: 07/26/2024] [Indexed: 08/23/2024]
Abstract
As an atomically thin electric conductor with a low density of highly mobile charge carriers, graphene is a suitable transducer for molecular adsorption. In this study, we demonstrate that the adsorption properties can be significantly enhanced with a laser-deposited TiO2 nanolayer on top of single-layer CVD graphene, whereas the effective charge transfer between the TiO2-adsorbed gas molecules and graphene is retained through the interface. The formation of such a heterostructure with optimally a monolayer thick oxide combined with ultraviolet irradiation (wavelength 365 nm, intensity <1 mW/mm2) dramatically enhances the gas-sensing properties. It provides an outstanding sensitivity for detecting NO2 in the range of a few ppb to a few hundred ppb-s in air, with response times below 30 s at room temperature. The effect of visible light (436 and 546 nm) was much weaker, indicating that the excitations due to light absorption in TiO2 play an essential role, while the characteristics of gas responses imply the involvement of both photoinduced adsorption and desorption. The sensing mechanism was confirmed by theoretical simulations on a NO2@Ti8O16C50 complex under periodic boundary conditions. The proposed sensor structure has significant additional merits, such as relative insensitivity to other polluting gases (CO, SO2, NH3) and air humidity, as well as long-term stability (>2 years) in ambient air. The results pave the way for an emerging class of gas sensor structures based on stacked 2D materials incorporating highly charge-sensitive transducer and selective receptor layers.
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Affiliation(s)
- Artjom Berholts
- Institute of Physics, University of Tartu, W. Ostwald Street 1, Tartu 50411, Estonia
| | - Margus Kodu
- Institute of Physics, University of Tartu, W. Ostwald Street 1, Tartu 50411, Estonia
| | - Pavel Rubin
- Institute of Physics, University of Tartu, W. Ostwald Street 1, Tartu 50411, Estonia
| | - Tauno Kahro
- Institute of Physics, University of Tartu, W. Ostwald Street 1, Tartu 50411, Estonia
| | - Harry Alles
- Institute of Physics, University of Tartu, W. Ostwald Street 1, Tartu 50411, Estonia
| | - Raivo Jaaniso
- Institute of Physics, University of Tartu, W. Ostwald Street 1, Tartu 50411, Estonia
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Mounasamy V, Mani GK, Madanagurusamy S. Vanadium oxide nanostructures for chemiresistive gas and vapour sensing: a review on state of the art. Mikrochim Acta 2020; 187:253. [DOI: 10.1007/s00604-020-4182-2] [Citation(s) in RCA: 23] [Impact Index Per Article: 5.8] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/19/2019] [Accepted: 02/24/2020] [Indexed: 02/02/2023]
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Guo Y, Sun X, Jiang J, Wang B, Chen X, Yin X, Qi W, Gao L, Zhang L, Lu Z, Jia R, Pendse S, Hu Y, Chen Z, Wertz E, Gall D, Feng J, Lu TM, Shi J. A Reconfigurable Remotely Epitaxial VO 2 Electrical Heterostructure. NANO LETTERS 2020; 20:33-42. [PMID: 31769995 DOI: 10.1021/acs.nanolett.9b02696] [Citation(s) in RCA: 6] [Impact Index Per Article: 1.5] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/10/2023]
Abstract
The reconfigurability of the electrical heterostructure featured with external variables, such as temperature, voltage, and strain, enabled electronic/optical phase transition in functional layers has great potential for future photonics, computing, and adaptive circuits. VO2 has been regarded as an archetypal phase transition building block with superior metal-insulator transition characteristics. However, the reconfigurable VO2-based heterostructure and the associated devices are rare due to the fundamental challenge in integrating high-quality VO2 in technologically important substrates. In this report, for the first time, we show the remote epitaxy of VO2 and the demonstration of a vertical diode device in a graphene/epitaxial VO2/single-crystalline BN/graphite structure with VO2 as a reconfigurable phase-change material and hexagonal boron nitride (h-BN) as an insulating layer. By diffraction and electrical transport studies, we show that the remote epitaxial VO2 films exhibit higher structural and electrical quality than direct epitaxial ones. By high-resolution transmission electron microscopy and Cs-corrected scanning transmission electron microscopy, we show that a graphene buffered substrate leads to a less strained VO2 film than the bare substrate. In the reconfigurable diode, we find that the Fermi level change and spectral weight shift along with the metal-insulator transition of VO2 could modify the transport characteristics. The work suggests the feasibility of developing a single-crystalline VO2-based reconfigurable heterostructure with arbitrary substrates and sheds light on designing novel adaptive photonics and electrical devices and circuits.
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Affiliation(s)
- Yuwei Guo
- Department of Materials Science and Engineering , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Xin Sun
- Department of Physics, Applied Physics, and Astronomy , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Jie Jiang
- Department of Materials Science and Engineering , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
- Faculty of Material Science and Engineering , Kunming University of Science and Technology , Kunming 650093 , China
| | - Baiwei Wang
- Department of Materials Science and Engineering , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Xinchun Chen
- State Key Laboratory of Tribology , Tsinghua University , Beijing 100084 , China
| | - Xuan Yin
- State Key Laboratory of Tribology , Tsinghua University , Beijing 100084 , China
| | - Wei Qi
- State Key Laboratory of Tribology , Tsinghua University , Beijing 100084 , China
| | - Lei Gao
- Beijing Advanced Innovation Center for Materials Genome Engineering, Institute for Advanced Materials and Technology , University of Science and Technology Beijing , Beijing , 100083 , China
| | - Lifu Zhang
- Department of Materials Science and Engineering , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Zonghuan Lu
- Department of Physics, Applied Physics, and Astronomy , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Ru Jia
- Department of Materials Science and Engineering , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Saloni Pendse
- Department of Materials Science and Engineering , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Yang Hu
- Department of Materials Science and Engineering , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
- Department of Physics, Applied Physics, and Astronomy , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Zhizhong Chen
- Department of Materials Science and Engineering , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Esther Wertz
- Department of Physics, Applied Physics, and Astronomy , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Daniel Gall
- Department of Materials Science and Engineering , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Jing Feng
- Faculty of Material Science and Engineering , Kunming University of Science and Technology , Kunming 650093 , China
| | - Toh-Ming Lu
- Department of Physics, Applied Physics, and Astronomy , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
| | - Jian Shi
- Department of Materials Science and Engineering , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
- Center for Materials, Devices, and Integrated Systems , Rensselaer Polytechnic Institute , Troy , New York 12180 , United States
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Khambalkar V, Birajdar S, Adhyapak P, Kulkarni S. Nanocomposite of polypyrrol and silica rods-gold nanoparticles core-shell as an ammonia sensor. NANOTECHNOLOGY 2019; 30:105501. [PMID: 30540977 DOI: 10.1088/1361-6528/aaf83d] [Citation(s) in RCA: 7] [Impact Index Per Article: 1.4] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/09/2023]
Abstract
Ammonia is widely needed in the chemical industry as well as in fertilizers for agriculture. However, in small as well as large quantities, it is not only hazardous for human health but also for our ecosystem. Therefore, ammonia sensing at low concentration with high sensitivity, selectivity and low response time as well as recovery time is important. Here, various nanosensors are fabricated using gold nanoparticles (∼15 nm), silica-gold nanoparticles coreshell particles and coreshell particles embedded in polypyrrol. Comparisons with bare polypyrrol and coreshell particles are also made. In fact, two types of coreshell particles with rod (∼300 nm × 2 μm) shape and spheres (200 nm) of silica were used to anchor gold nanoparticles on them. A comparison showed that silica-gold core-shell particle with silica rods had the highest sensitivity (∼166% @ 130 ppm) amongst all. The sensor is simple to operate (only resistance change is measured), requires no heater as the sensing occurs at room temperature, and showed no response, except for ammonia, to other gases or humidity. It also has a low response time (4 s) and recovery time (10 s) at the lowest (10 ppm) ammonia concentration measured here. Thus, a simple, economical ammonia sensor has been demonstrated here.
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Affiliation(s)
- Vaibhav Khambalkar
- Indian Institute of Science Education and Research, Pune, Dr Homi Bhabha Road, Pune-411008, India
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Kodu M, Berholts A, Kahro T, Eriksson J, Yakimova R, Avarmaa T, Renge I, Alles H, Jaaniso R. Graphene-Based Ammonia Sensors Functionalised with Sub-Monolayer V₂O₅: A Comparative Study of Chemical Vapour Deposited and Epitaxial Graphene †. SENSORS 2019; 19:s19040951. [PMID: 30813421 PMCID: PMC6413083 DOI: 10.3390/s19040951] [Citation(s) in RCA: 17] [Impact Index Per Article: 3.4] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 01/08/2019] [Revised: 02/15/2019] [Accepted: 02/19/2019] [Indexed: 01/25/2023]
Abstract
Graphene in its pristine form has demonstrated a gas detection ability in an inert carrier gas. For practical use in ambient atmosphere, its sensor properties should be enhanced with functionalisation by defects and dopants, or by decoration with nanophases of metals or/and metal oxides. Excellent sensor behaviour was found for two types of single layer graphenes: grown by chemical vapour deposition (CVD) and transferred onto oxidized silicon (Si/SiO2/CVDG), and the epitaxial graphene grown on SiC (SiC/EG). Both graphene samples were functionalised using a pulsed laser deposited (PLD) thin V2O5 layer of average thickness ≈ 0.6 nm. According to the Raman spectra, the SiC/EG has a remarkable resistance against structural damage under the laser deposition conditions. By contrast, the PLD process readily induces defects in CVD graphene. Both sensors showed remarkable and selective sensing of NH3 gas in terms of response amplitude and speed, as well as recovery rate. SiC/EG showed a response that was an order of magnitude larger as compared to similarly functionalised CVDG sensor (295% vs. 31% for 100 ppm NH3). The adsorption site properties are assigned to deposited V2O5 nanophase, being similar for both sensors, rather than (defect) graphene itself. The substantially larger response of SiC/EG sensor is probably the result of the smaller initial free charge carrier doping in EG.
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Affiliation(s)
- Margus Kodu
- Institute of Physics, University of Tartu, W. Ostwald Street 1, EE50411 Tartu, Estonia.
| | - Artjom Berholts
- Institute of Physics, University of Tartu, W. Ostwald Street 1, EE50411 Tartu, Estonia.
| | - Tauno Kahro
- Institute of Physics, University of Tartu, W. Ostwald Street 1, EE50411 Tartu, Estonia.
| | - Jens Eriksson
- Department of Physics, Chemistry and Biology, Linköping University, 58183 Linköping, Sweden.
| | - Rositsa Yakimova
- Department of Physics, Chemistry and Biology, Linköping University, 58183 Linköping, Sweden.
| | - Tea Avarmaa
- Institute of Physics, University of Tartu, W. Ostwald Street 1, EE50411 Tartu, Estonia.
| | - Indrek Renge
- Institute of Physics, University of Tartu, W. Ostwald Street 1, EE50411 Tartu, Estonia.
| | - Harry Alles
- Institute of Physics, University of Tartu, W. Ostwald Street 1, EE50411 Tartu, Estonia.
| | - Raivo Jaaniso
- Institute of Physics, University of Tartu, W. Ostwald Street 1, EE50411 Tartu, Estonia.
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Birajdar SN, Hebalkar NY, Pardeshi SK, Kulkarni SK, Adhyapak PV. Ruthenium-decorated vanadium pentoxide for room temperature ammonia sensing. RSC Adv 2019; 9:28735-28745. [PMID: 35529636 PMCID: PMC9071197 DOI: 10.1039/c9ra04382a] [Citation(s) in RCA: 12] [Impact Index Per Article: 2.4] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/11/2019] [Accepted: 08/31/2019] [Indexed: 12/31/2022] Open
Abstract
Layer structured vanadium pentoxide (V2O5) microparticles were synthesized hydrothermally and successfully decorated by a facile wet chemical route, with ∼10–20 nm sized ruthenium nanoparticles. Both V2O5 and ruthenium nanoparticle decorated V2O5 (1%Ru@V2O5) were investigated for their suitability as resistive gas sensors. It was found that the 1%Ru@V2O5 sample showed very high selectivity and sensitivity towards ammonia vapors. The sensitivity measurements were carried out at 30 °C (room temperature), 50 °C and 100 °C. The best results were obtained at room temperature for 1%Ru@V2O5. Remarkably as short a response time as 0.52 s @ 130 ppm and as low as 9.39 s @ 10 ppm recovery time at room temperature along with high selectivity towards many gases and vapors have been noted in the 10 to 130 ppm ammonia concentration range. Short response and recovery time, high reproducibility, selectivity and room temperature operation are the main attributes of the 1%Ru@V2O5 sensor. Higher sensitivity of 1%Ru@V2O5 compared to V2O5 has been explained and is due to dissociation of atmospheric water molecules on 1%Ru@V2O5 as compared to bare V2O5 which makes hydrogen atoms available on Brønsted sites for ammonia adsorption and sensing. The presence of ruthenium with a thin layer of oxide is clear from X-ray photoelectron spectroscopy and that of water molecules from Fourier transform infrared spectroscopy. Layer structured vanadium pentoxide (V2O5) microparticles were synthesized hydrothermally and successfully decorated by a facile wet chemical route, with ∼10–20 nm sized ruthenium nanoparticles.![]()
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Affiliation(s)
| | - Neha Y. Hebalkar
- International Advanced Research Centre for Powder Metallurgy and New Materials
- Hyderabad-500005
- India
| | | | | | - Parag V. Adhyapak
- Centre for Materials for Electronics Technology (C-MET)
- Pune-411008
- India
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Liu M, Chen Y, Qin C, Zhang Z, Ma S, Cai X, Li X, Wang Y. Electrodeposition of reduced graphene oxide with chitosan based on the coordination deposition method. BEILSTEIN JOURNAL OF NANOTECHNOLOGY 2018; 9:1200-1210. [PMID: 29765797 PMCID: PMC5942374 DOI: 10.3762/bjnano.9.111] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/29/2017] [Accepted: 03/16/2018] [Indexed: 05/03/2023]
Abstract
The electrodeposition of graphene has drawn considerable attention due to its appealing applications for sensors, supercapacitors and lithium-ion batteries. However, there are still some limitations in the current electrodeposition methods for graphene. Here, we present a novel electrodeposition method for the direct deposition of reduced graphene oxide (rGO) with chitosan. In this method, a 2-hydroxypropyltrimethylammonium chloride-based chitosan-modified rGO material was prepared. This material disperses homogenously in the chitosan solution, forming a deposition solution with good dispersion stability. Subsequently, the modified rGO material was deposited on an electrode through codeposition with chitosan, based on the coordination deposition method. After electrodeposition, the homogeneous, deposited rGO/chitosan films can be generated on copper or silver electrodes or substrates. The electrodeposition method allows for the convenient and controlled creation of rGO/chitosan nanocomposite coatings and films of different shapes and thickness. It also introduces a new method of creating films, as they can be peeled completely from the electrodes. Moreover, this method allows for a rGO/chitosan film to be deposited directly onto an electrode, which can then be used for electrochemical detection.
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Affiliation(s)
- Mingyang Liu
- School of Materials Science and Engineering, Wuhan University of Technology, 122 Luoshi Road, Wuhan 430070, China
| | - Yanjun Chen
- School of Materials Science and Engineering, Wuhan University of Technology, 122 Luoshi Road, Wuhan 430070, China
| | - Chaoran Qin
- School of Materials Science and Engineering, Wuhan University of Technology, 122 Luoshi Road, Wuhan 430070, China
| | - Zheng Zhang
- School of Materials Science and Engineering, Wuhan University of Technology, 122 Luoshi Road, Wuhan 430070, China
| | - Shuai Ma
- School of Materials Science and Engineering, Wuhan University of Technology, 122 Luoshi Road, Wuhan 430070, China
| | - Xiuru Cai
- School of Materials Science and Engineering, Wuhan University of Technology, 122 Luoshi Road, Wuhan 430070, China
| | - Xueqian Li
- School of Materials Science and Engineering, Wuhan University of Technology, 122 Luoshi Road, Wuhan 430070, China
| | - Yifeng Wang
- School of Materials Science and Engineering, Wuhan University of Technology, 122 Luoshi Road, Wuhan 430070, China
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