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Effect of boron doping on the structural, optical and electrical properties of ZnO nanoparticles produced by the hydrothermal method

dc.contributor.authorŞenol, Sevim Demirözü
dc.contributor.authorÖztürk, Özgür
dc.contributor.authorTerzioğlu, Cabir
dc.date.accessioned2026-01-02T23:28:51Z
dc.date.issued2015-11-01
dc.description.abstractAbstract The effect of boron doping with 0–11 at% concentration on structural, optical and electrical properties of zinc oxide nanopowder synthesized by a hydrothermal method has been reported. We have performed X-Ray Diffraction (XRD), Scanning Electron Microscopy (SEM), optical, Hall and resistivity measurements on the samples. XRD results reveal that all B doped ZnO nanopowders have single phase hexagonal (Wurtzite) structure without any impurity. But the positions of main diffracted peaks of ZnO shifted slightly towards small (2 θ ) angle and grain size decreases from 60.75 nm to 34.34 nm with an increase of B doping concentrations. SEM analysis indicates that the doping concentration of B affected the surface morphology of ZnO nanostructures. Optical properties were examined by UV–vis absorption/diffuse reflectance spectroscopy. The optical band gap of Zn 1− x B x O nanostructures increased from 3.27 eV to 3.30 eV with increasing doping from x =0 to x =0.11. The role of doping concentrations of B on the transport properties was searched by temperature dependent Hall measurements in 180–350 K temperature range. The carrier concentration of the samples increased from 0.11×10 14  cm −3 to 4.08×10 14  cm −3 , the Hall mobility decreased from 5.61 cm 2  V −1  s −1 to 1.22 cm 2  V −1  s −1 and electrical resistivity decreased from 10.89×10 4  Ω cm to 1.25×10 4  Ω cm with the increase of the B doping concentrations at room temperature. The electrical resistivity is observed to decrease with both the increase in dopant concentration and the temperature in the range of 180–350 K.
dc.description.urihttps://doi.org/10.1016/j.ceramint.2015.05.069
dc.description.urihttps://dx.doi.org/10.1016/j.ceramint.2015.05.069
dc.description.urihttps://hdl.handle.net/20.500.12491/8170
dc.identifier.doi10.1016/j.ceramint.2015.05.069
dc.identifier.endpage11201
dc.identifier.issn0272-8842
dc.identifier.openairedoi_dedup___::88e2f495e3bbe3d61f555fda3dad9400
dc.identifier.orcid0000-0002-5322-963x
dc.identifier.scopus2-s2.0-84930738080
dc.identifier.startpage11194
dc.identifier.urihttps://hdl.handle.net/20.500.12597/36047
dc.identifier.volume41
dc.identifier.wos000359165500108
dc.language.isoeng
dc.publisherElsevier BV
dc.relation.ispartofCeramics International
dc.rightsOPEN
dc.subjectHall Effect Measurements
dc.subjectB-doped ZnO
dc.subjectHydrothermal Method
dc.subjectOptical Properties
dc.titleEffect of boron doping on the structural, optical and electrical properties of ZnO nanoparticles produced by the hydrothermal method
dc.typeArticle
dspace.entity.typePublication
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We have performed X-Ray Diffraction (XRD), Scanning Electron Microscopy (SEM), optical, Hall and resistivity measurements on the samples. XRD results reveal that all B doped ZnO nanopowders have single phase hexagonal (Wurtzite) structure without any impurity. But the positions of main diffracted peaks of ZnO shifted slightly towards small (2 θ ) angle and grain size decreases from 60.75 nm to 34.34 nm with an increase of B doping concentrations. SEM analysis indicates that the doping concentration of B affected the surface morphology of ZnO nanostructures. Optical properties were examined by UV–vis absorption/diffuse reflectance spectroscopy. The optical band gap of Zn 1− x B x O nanostructures increased from 3.27 eV to 3.30 eV with increasing doping from x =0 to x =0.11. The role of doping concentrations of B on the transport properties was searched by temperature dependent Hall measurements in 180–350 K temperature range. 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