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Effect of Ni and Al doping on structural, optical, and CO2 gas sensing properties of 1D ZnO nanorods produced by hydrothermal method

dc.contributor.authorBulut, Fatih
dc.contributor.authorOzturk, Özgür
dc.contributor.authorAcar, Selim
dc.contributor.authorYildirim, Gürcan
dc.date.accessioned2026-01-04T16:01:26Z
dc.date.issued2021-12-09
dc.description.abstractAbstractIn the present study, the one‐dimensional ZnO nanorod structures are produced within the different nickel and aluminum molecular weight ratios of 0–7% using the hydrothermal method. It is found that the aluminum (Al) and nickel (Ni) impurities with different ionic radius, chemical valence, and electron configurations of outer shell cause to vary the fundamental characteristic features including the crystallinity quality, crystallite size, surface morphology, nanorod diameter, optical absorbance, energy band gap, resistance, gas response, and gas sensing properties. The structural analyses performed by powder X‐ray diffraction (XRD) and scanning electron microscopy (SEM) indicate that the samples are found to crystallize in the hexagonal wurtzite structure. The presence of optimum nickel and aluminum in the crystal system improves considerably the crystallinity quality and surface morphology. Additionally, the combination of electron dispersive X‐ray (EDX) and XRD results declare that the Ni and Al impurities incorporate successfully into the ZnO crystal structure. Moreover, the diameters of nanorod structures in 1D orientation are determined to be 80 nm or below. The hexagonal wurtzite‐type ZnO nanorod structure prepared by 5% Ni has more space between the nanorods and thus presents higher response to the CO2 detection. Further, the optical absorbance spectra display that the band gap value is observed to decrease regularly with the increment in the doping level as a result of band shrinkage effect depending on the enhancement of mobile hole carrier concentrations in the crystal structure. In other words, the doping mechanism leads to vary the homogeneities in the interfacial charges, nanorod diameters, ZnO oxide layer composition and thickness. The last test conducted in this study is responsible for the determination of CO2 gas sensing levels. The obtained gas sensing results are further compared with each other and literature findings. It is observed that 5% Ni‐doped sample provides more successful results than other samples in the sensing CO2 gas at the different concentrations. All in all, the paper establishing a strong methodology between doping mechanism and change in the fundamental characteristic features of hexagonal wurtzite‐type ZnO with the aid of advanced microscopy techniques will become pioneering research to answer key questions in materials sciences and electronic research.
dc.description.urihttps://doi.org/10.1002/jemt.24013
dc.description.urihttps://pubmed.ncbi.nlm.nih.gov/34882897
dc.description.urihttps://avesis.gazi.edu.tr/publication/details/2c51ef8c-9be1-465c-acdc-4682d8bbc991/oai
dc.description.urihttps://hdl.handle.net/20.500.12491/11131
dc.description.urihttps://hdl.handle.net/11486/7294
dc.identifier.doi10.1002/jemt.24013
dc.identifier.eissn1097-0029
dc.identifier.endpage1517
dc.identifier.issn1059-910X
dc.identifier.openairedoi_dedup___::c02d98b6ba2de6aca967ba02cb863f64
dc.identifier.orcid0000-0001-5335-2307
dc.identifier.orcid0000-0002-0391-5551
dc.identifier.orcid0000-0003-4014-7800
dc.identifier.orcid0000-0002-5177-3703
dc.identifier.pubmed34882897
dc.identifier.scopus2-s2.0-85120812878
dc.identifier.startpage1502
dc.identifier.urihttps://hdl.handle.net/20.500.12597/39220
dc.identifier.volume85
dc.identifier.wos000728175300001
dc.language.isoeng
dc.publisherWiley
dc.relation.ispartofMicroscopy Research and Technique
dc.rightsOPEN
dc.subjectCO2 Gas Sensing
dc.subjecthydrothermal
dc.subjectnickel doped
dc.subjectHydrothermal
dc.subjectNickel Doped
dc.subjectAluminum Doped
dc.subjectaluminum doped
dc.subjectZinc Oxide Nanorod
dc.subjectzinc oxide nanorod
dc.subjectCO2 gas sensing
dc.titleEffect of Ni and Al doping on structural, optical, and CO2 gas sensing properties of 1D ZnO nanorods produced by hydrothermal method
dc.typeArticle
dspace.entity.typePublication
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It is found that the aluminum (Al) and nickel (Ni) impurities with different ionic radius, chemical valence, and electron configurations of outer shell cause to vary the fundamental characteristic features including the crystallinity quality, crystallite size, surface morphology, nanorod diameter, optical absorbance, energy band gap, resistance, gas response, and gas sensing properties. The structural analyses performed by powder X‐ray diffraction (XRD) and scanning electron microscopy (SEM) indicate that the samples are found to crystallize in the hexagonal wurtzite structure. The presence of optimum nickel and aluminum in the crystal system improves considerably the crystallinity quality and surface morphology. Additionally, the combination of electron dispersive X‐ray (EDX) and XRD results declare that the Ni and Al impurities incorporate successfully into the ZnO crystal structure. Moreover, the diameters of nanorod structures in 1D orientation are determined to be 80 nm or below. The hexagonal wurtzite‐type ZnO nanorod structure prepared by 5% Ni has more space between the nanorods and thus presents higher response to the CO<jats:sub>2</jats:sub> detection. Further, the optical absorbance spectra display that the band gap value is observed to decrease regularly with the increment in the doping level as a result of band shrinkage effect depending on the enhancement of mobile hole carrier concentrations in the crystal structure. In other words, the doping mechanism leads to vary the homogeneities in the interfacial charges, nanorod diameters, ZnO oxide layer composition and thickness. The last test conducted in this study is responsible for the determination of CO<jats:sub>2</jats:sub> gas sensing levels. The obtained gas sensing results are further compared with each other and literature findings. It is observed that 5% Ni‐doped sample provides more successful results than other samples in the sensing CO<jats:sub>2</jats:sub> gas at the different concentrations. All in all, the paper establishing a strong methodology between doping mechanism and change in the fundamental characteristic features of hexagonal wurtzite‐type ZnO with the aid of advanced microscopy techniques will become pioneering research to answer key questions in materials sciences and electronic research.</jats:p>"],"publicationDate":"2021-12-09","publisher":"Wiley","embargoEndDate":null,"sources":["Crossref"],"formats":["application/pdf"],"contributors":["Bolu Abant İzzet Baysal University Institutional Repository"],"coverages":null,"bestAccessRight":{"code":"c_abf2","label":"OPEN","scheme":"http://vocabularies.coar-repositories.org/documentation/access_rights/"},"container":{"name":"Microscopy Research and Technique","issnPrinted":"1059-910X","issnOnline":"1097-0029","issnLinking":null,"ep":"1517","iss":null,"sp":"1502","vol":"85","edition":null,"conferencePlace":null,"conferenceDate":null},"documentationUrls":null,"codeRepositoryUrl":null,"programmingLanguage":null,"contactPeople":null,"contactGroups":null,"tools":null,"size":null,"version":null,"geoLocations":null,"id":"doi_dedup___::c02d98b6ba2de6aca967ba02cb863f64","originalIds":["10.1002/jemt.24013","50|doiboost____|c02d98b6ba2de6aca967ba02cb863f64","34882897","50|od_____10046::6a7ca6c0c02bb442c3ac6833c244add9","2c51ef8c-9be1-465c-acdc-4682d8bbc991","oai:acikerisim.ibu.edu.tr:20.500.12491/11131","50|od_____10075::7f0b47f722d1954f6300b97c7487c3c2","50|od______3302::287b23815ccacb1b89b1d610a60cc0fa","oai:acikerisim.sinop.edu.tr:11486/7294"],"pids":[{"scheme":"doi","value":"10.1002/jemt.24013"},{"scheme":"pmid","value":"34882897"},{"scheme":"handle","value":"20.500.12491/11131"},{"scheme":"handle","value":"11486/7294"}],"dateOfCollection":null,"lastUpdateTimeStamp":null,"indicators":{"citationImpact":{"citationCount":8,"influence":2.7911895e-9,"popularity":7.8785956e-9,"impulse":8,"citationClass":"C5","influenceClass":"C5","impulseClass":"C4","popularityClass":"C4"}},"instances":[{"pids":[{"scheme":"doi","value":"10.1002/jemt.24013"}],"license":"Wiley Online Library User Agreement","type":"Article","urls":["https://doi.org/10.1002/jemt.24013"],"publicationDate":"2021-12-09","refereed":"peerReviewed"},{"pids":[{"scheme":"pmid","value":"34882897"}],"alternateIdentifiers":[{"scheme":"doi","value":"10.1002/jemt.24013"}],"type":"Article","urls":["https://pubmed.ncbi.nlm.nih.gov/34882897"],"refereed":"nonPeerReviewed"},{"alternateIdentifiers":[{"scheme":"doi","value":"10.1002/jemt.24013"}],"type":"Article","urls":["https://avesis.gazi.edu.tr/publication/details/2c51ef8c-9be1-465c-acdc-4682d8bbc991/oai"],"publicationDate":"2022-04-01","refereed":"nonPeerReviewed"},{"pids":[{"scheme":"handle","value":"20.500.12491/11131"}],"alternateIdentifiers":[{"scheme":"doi","value":"10.1002/jemt.24013"}],"type":"Article","urls":["https://doi.org/10.1002/jemt.24013","https://hdl.handle.net/20.500.12491/11131"],"publicationDate":"2022-01-01","refereed":"nonPeerReviewed"},{"pids":[{"scheme":"handle","value":"11486/7294"}],"alternateIdentifiers":[{"scheme":"doi","value":"10.1002/jemt.24013"}],"type":"Article","urls":["https://hdl.handle.net/11486/7294","https://doi.org/10.1002/jemt.24013"],"publicationDate":"2025-03-23","refereed":"nonPeerReviewed"}],"isGreen":true,"isInDiamondJournal":false}
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