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Conversion from p- to n-Type Conductivity in CuO Thin Films Through Zr Doping

CuO films with Zr doping were successfully fabricated on substrates of soda-lime glass (SLG) using a spin-coating method at various doping concentrations. X-ray diffraction (XRD) patterns for pure and Zr-doped CuO thin films indicated that all thin CuO films have a monoclinic polycrystalline nature,...

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Published in:Journal of electronic materials 2022-10, Vol.51 (10), p.5644-5654
Main Author: Baturay, Şilan
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description CuO films with Zr doping were successfully fabricated on substrates of soda-lime glass (SLG) using a spin-coating method at various doping concentrations. X-ray diffraction (XRD) patterns for pure and Zr-doped CuO thin films indicated that all thin CuO films have a monoclinic polycrystalline nature, with two maximum peaks (−111) and (111). The dislocation density values of the (−111) and (111) planes are increased from 13.4 × 10 14 to 34.9 × 10 14  m −2 and from 26 × 10 14 to 42.7 × 10 14  m −2 , respectively, owing to the expansion of structural parameters with Zr dopant content. Scanning electron microscopy (SEM) indicated nanostructure particles uniformly distributed on all thin-film surfaces without any agglomerated nanostructure particles. The thickness of CuO films in conjunction with Zr doping is approximately 460 nm. The EDX spectrum of pure CuO in thin film contains Cu and O elements; 1%, 2%, and 3% Zr-doped CuO thin films contain Zr, Cu, and O elements, as expected. Atomic force microscopy (AFM) figures indicate that the surface topologies of thin films are uniformly distributed. Ultraviolet–visible spectroscopy (UV–Vis) measurements of the thin films revealed that the transmittance increased from 25% to 45% in the visible range with increasing Zr concentration at room temperature. The energy band gap increased from 1.67 to 2.03 eV with increasing Zr concentration. At room temperature, a Hall effect system was used to investigate the electrical parameters, including carrier concentration, resistivity, conductivity type, and hole mobility of the CuO films with Zr doping. Conductivity type conversion was observed with 2% and 3% Zr-doped CuO, and confirmed by capacity–voltage ( C - V ) measurements. The charge-carrier concentration of the samples ranged from 1.08 × 10 16 to 5.06 × 10 18  cm −3 with Zr doping. Thus, the optical and electrical properties of CuO thin film such as the band gap energy, transmittance, and carrier mobility can be modified. Graphical Abstract
doi_str_mv 10.1007/s11664-022-09836-9
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X-ray diffraction (XRD) patterns for pure and Zr-doped CuO thin films indicated that all thin CuO films have a monoclinic polycrystalline nature, with two maximum peaks (−111) and (111). The dislocation density values of the (−111) and (111) planes are increased from 13.4 × 10 14 to 34.9 × 10 14  m −2 and from 26 × 10 14 to 42.7 × 10 14  m −2 , respectively, owing to the expansion of structural parameters with Zr dopant content. Scanning electron microscopy (SEM) indicated nanostructure particles uniformly distributed on all thin-film surfaces without any agglomerated nanostructure particles. The thickness of CuO films in conjunction with Zr doping is approximately 460 nm. The EDX spectrum of pure CuO in thin film contains Cu and O elements; 1%, 2%, and 3% Zr-doped CuO thin films contain Zr, Cu, and O elements, as expected. Atomic force microscopy (AFM) figures indicate that the surface topologies of thin films are uniformly distributed. Ultraviolet–visible spectroscopy (UV–Vis) measurements of the thin films revealed that the transmittance increased from 25% to 45% in the visible range with increasing Zr concentration at room temperature. The energy band gap increased from 1.67 to 2.03 eV with increasing Zr concentration. At room temperature, a Hall effect system was used to investigate the electrical parameters, including carrier concentration, resistivity, conductivity type, and hole mobility of the CuO films with Zr doping. Conductivity type conversion was observed with 2% and 3% Zr-doped CuO, and confirmed by capacity–voltage ( C - V ) measurements. The charge-carrier concentration of the samples ranged from 1.08 × 10 16 to 5.06 × 10 18  cm −3 with Zr doping. Thus, the optical and electrical properties of CuO thin film such as the band gap energy, transmittance, and carrier mobility can be modified. 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Electron. Mater</addtitle><description>CuO films with Zr doping were successfully fabricated on substrates of soda-lime glass (SLG) using a spin-coating method at various doping concentrations. X-ray diffraction (XRD) patterns for pure and Zr-doped CuO thin films indicated that all thin CuO films have a monoclinic polycrystalline nature, with two maximum peaks (−111) and (111). The dislocation density values of the (−111) and (111) planes are increased from 13.4 × 10 14 to 34.9 × 10 14  m −2 and from 26 × 10 14 to 42.7 × 10 14  m −2 , respectively, owing to the expansion of structural parameters with Zr dopant content. Scanning electron microscopy (SEM) indicated nanostructure particles uniformly distributed on all thin-film surfaces without any agglomerated nanostructure particles. The thickness of CuO films in conjunction with Zr doping is approximately 460 nm. The EDX spectrum of pure CuO in thin film contains Cu and O elements; 1%, 2%, and 3% Zr-doped CuO thin films contain Zr, Cu, and O elements, as expected. Atomic force microscopy (AFM) figures indicate that the surface topologies of thin films are uniformly distributed. Ultraviolet–visible spectroscopy (UV–Vis) measurements of the thin films revealed that the transmittance increased from 25% to 45% in the visible range with increasing Zr concentration at room temperature. The energy band gap increased from 1.67 to 2.03 eV with increasing Zr concentration. At room temperature, a Hall effect system was used to investigate the electrical parameters, including carrier concentration, resistivity, conductivity type, and hole mobility of the CuO films with Zr doping. Conductivity type conversion was observed with 2% and 3% Zr-doped CuO, and confirmed by capacity–voltage ( C - V ) measurements. The charge-carrier concentration of the samples ranged from 1.08 × 10 16 to 5.06 × 10 18  cm −3 with Zr doping. Thus, the optical and electrical properties of CuO thin film such as the band gap energy, transmittance, and carrier mobility can be modified. 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Electron. Mater</stitle><date>2022-10-01</date><risdate>2022</risdate><volume>51</volume><issue>10</issue><spage>5644</spage><epage>5654</epage><pages>5644-5654</pages><issn>0361-5235</issn><eissn>1543-186X</eissn><abstract>CuO films with Zr doping were successfully fabricated on substrates of soda-lime glass (SLG) using a spin-coating method at various doping concentrations. X-ray diffraction (XRD) patterns for pure and Zr-doped CuO thin films indicated that all thin CuO films have a monoclinic polycrystalline nature, with two maximum peaks (−111) and (111). The dislocation density values of the (−111) and (111) planes are increased from 13.4 × 10 14 to 34.9 × 10 14  m −2 and from 26 × 10 14 to 42.7 × 10 14  m −2 , respectively, owing to the expansion of structural parameters with Zr dopant content. Scanning electron microscopy (SEM) indicated nanostructure particles uniformly distributed on all thin-film surfaces without any agglomerated nanostructure particles. The thickness of CuO films in conjunction with Zr doping is approximately 460 nm. The EDX spectrum of pure CuO in thin film contains Cu and O elements; 1%, 2%, and 3% Zr-doped CuO thin films contain Zr, Cu, and O elements, as expected. Atomic force microscopy (AFM) figures indicate that the surface topologies of thin films are uniformly distributed. Ultraviolet–visible spectroscopy (UV–Vis) measurements of the thin films revealed that the transmittance increased from 25% to 45% in the visible range with increasing Zr concentration at room temperature. The energy band gap increased from 1.67 to 2.03 eV with increasing Zr concentration. At room temperature, a Hall effect system was used to investigate the electrical parameters, including carrier concentration, resistivity, conductivity type, and hole mobility of the CuO films with Zr doping. Conductivity type conversion was observed with 2% and 3% Zr-doped CuO, and confirmed by capacity–voltage ( C - V ) measurements. The charge-carrier concentration of the samples ranged from 1.08 × 10 16 to 5.06 × 10 18  cm −3 with Zr doping. Thus, the optical and electrical properties of CuO thin film such as the band gap energy, transmittance, and carrier mobility can be modified. Graphical Abstract</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s11664-022-09836-9</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0002-8122-6671</orcidid></addata></record>
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subjects Carrier density
Carrier mobility
Characterization and Evaluation of Materials
Chemistry and Materials Science
Conversion
Copper oxides
Current carriers
Diffraction patterns
Dislocation density
Doping
Electrical properties
Electrical resistivity
Electronics and Microelectronics
Energy bands
Energy gap
Hall effect
Hole mobility
Instrumentation
Materials Science
Microscopy
Nanostructure
Optical and Electronic Materials
Optical properties
Original Research Article
Parameters
Room temperature
Soda-lime glass
Solid State Physics
Spin coating
Thickness
Thin films
Topology
Transmittance
title Conversion from p- to n-Type Conductivity in CuO Thin Films Through Zr Doping
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