• Title/Summary/Keyword: Photoluminescence spectroscopy

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Preparation of SiO2-Coated TiO2 Composite Materials with Enhanced Photocatalytic Activity Under UV Light

  • Hu, Shaozheng;Li, Fayun;Fan, Zhiping
    • Bulletin of the Korean Chemical Society
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    • v.33 no.6
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    • pp.1895-1899
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    • 2012
  • $SiO_2$-coated $TiO_2$ composite materials with enhanced photocatalytic activity under UV light was prepared by a simple catalytic hydrolysis method. XRD, TEM, UV-vis spectroscopy, Photoluminescence, FT-IR and XP spectra were used to characterize the prepared samples. The obvious shell-core structure was shown for obtained $SiO_2$@$TiO_2$ sample. The average thickness of the $SiO_2$ coating layer was 2-3 nm. The interaction between $SiO_2$ and $TiO_2$ restrained the recombination of excited electrons and holes. The photocatalytic activities were tested in the degradation of an aqueous solution of a reactive dyestuff, methylene blue, under UV light. The photocatalytic activity of $SiO_2$@$TiO_2$ was much higher than that of P25 and mechanical mixing sample $SiO_2/TiO_2$. The possible mechanism for the photocatalysis was proposed.

Preparation of Gallium Nitride Powders and Nanowires from a Gallium(III) Nitrate Salt in Flowing Ammonia

  • Jung, Woo-Sik
    • Bulletin of the Korean Chemical Society
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    • v.25 no.1
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    • pp.51-54
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    • 2004
  • Gallium nitride (GaN) powders were prepared by calcining a gallium(III) nitrate salt in flowing ammonia in the temperature ranging from 500 to 1050 $^{\circ}C$. The process of conversion of the salt to GaN was monitored by X-ray diffraction and $^{71}Ga$ MAS (magic-angle spinning) NMR spectroscopy. The salt decomposed to ${\gamma}-Ga_2O_3$ and then converted to GaN without ${\gamma}-{\beta}Ga_2O_3$ phase transition. It is most likely that the conversion of ${\gamma}-Ga_2O_3$ to GaN does not proceed through $Ga_2O$ but stepwise via amorphous gallium oxynitride ($GaO_xN_y$) as intermediates. The GaN nanowires and microcrystals were obtained by calcining the pellet containing a mixture of ${\gamma}-Ga_2O_3$ and carbon in flowing ammonia at 900 $^{\circ}C$ for 15 h. The growth of the nanowire might be explained by the vapor-solid (VS) mechanism in a confined reactor. Room-temperature photoluminescence spectra of as-synthesized GaN powders obtained showed the emission peak at 363 nm.

Photocatalytic degradation and antibacterial investigation of nano synthesized Ag3VO4 particles @PAN nanofibers

  • Saud, Prem Singh;Ghouri, Zafar Khan;Pant, Bishweshwar;An, Taehee;Lee, Joong Hee;Park, Mira;Kim, Hak-Yong
    • Carbon letters
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    • v.18
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    • pp.30-36
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    • 2016
  • Well-dispersed Ag3VO4 nanoparticles @polyacrylonitrile (PAN) nanofibers were synthesized by an easily controlled, template-free method as a photo-catalyst for the degradation of methylene blue. Their structural, optical, and photocatalytic properties have been studied by X-ray diffraction, transmission electron microscopy, field-emission scanning electron microscopy equipped with rapid energy dispersive analysis of X-ray, photoluminescence, and ultraviolet-visible spectroscopy. The characterization procedures revealed that the obtained material is PAN nanofibers decorated by Ag3VO4 nanoparticles. Photocatalytic degradation of methylene blue investigated in an aqueous solution under irradiation showed 99% degradation of the dye within 75 min. Finally, the antibacterial performance of Ag3VO4 nanoparticles @PAN composite nanofibers was experimentally verified by the destruction of Escherichia coli. These results suggest that the developed inexpensive and functional nanomaterials can serve as a non-precious catalyst for environmental applications.

Enhanced Photocurrent from CdS Sensitized ZnO Nanorods

  • Nayak, Jhasaketan;Son, Min-Kyu;Kim, Jin-Kyoung;Kim, Soo-Kyoung;Lee, Jeong-Hoon;Kim, Hee-Je
    • Journal of Electrical Engineering and Technology
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    • v.7 no.6
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    • pp.965-970
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    • 2012
  • Structure and optical properties of cadmium sulphide-zinc oxide composite nanorods have been evaluated by suitable characterization techniques. The X-ray diffraction spectrum contains a series of peaks corresponding to reflections from various sets of lattice planes of hexagonal ZnO as well as CdS. The above observation is supported by the Micro-Raman spectroscopy result. The optical reflectance spectra of CdS-ZnO is compared with that of ZnO where we observe an enhanced absorption and hence diminished reflection from CdS-ZnO compared to that from only ZnO. A very small intensity of the visible photoluminescence peak observed at 550 nm proves that the ZnO nanorods have very low concentrations of point defects such as oxygen vacancies and zinc interstitials. The photocurrent in the visible region has been significantly enhanced due to deposition of CdS on the surface of the ZnO nanorods. CdS acts as a visible sensitizer because of its lower band gap compared to ZnO.

The Effect of the ZnO Nanorod Surface on the Optical Property (ZnO 나노막대의 표면이 광학적 특성에 미치는 영향)

  • Cho, Hyun-Min;Rhee, Seuk-Joo;Cho, Jae-Won
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.23 no.2
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    • pp.93-97
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    • 2010
  • We have studied the effect of the chemical composition of the ZnO nanorod surface on the optical characteristics. The surface was treated with H- and O-plasma at different surface temperatures. The chemical composition of the surface of the ZnO nanorod, being investigated by Auger Electron Spectroscopy(AES), was related to the Photoluminescence(PL) data reported in our previous results. The AES showed the opposite results for the $H_2$ and $O_2$ plasma treatments. The ratio of Zn to O on the surface of the ZnO nanorod increased in the case of $H_2$ plasma, while the composition rate of O increased after $O_2$ plasma treatment. The AES results seems to be correlated to the shift in PL peaks. The increase in the composition rate of Zn on the surface of ZnO nanorod is considered to cause the blue shift of the UV peak. On the contrary, the relative increase of O is considered to cause the red shift in PL peaks.

Properties of ZnO Thin Films Grown by Radio-frequency Magnetron Sputtering in terms of O2/Ar Mixture Flow Ratio (O2/Ar 혼합 유량비를 변수로 갖는 라디오파 마그네트론 스퍼터링으로 성장된 ZnO 박막의 특성)

  • Cho, Shin-Ho
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.20 no.11
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    • pp.932-938
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    • 2007
  • The structural, optical, and electrical properties of ZnO thin films grown on glass by radio-frequency (rf) magnetron sputtering were investigated. The mixture flow ratio of $O_2$ to Ar, which was operated with sputtering gas, was chosen as a parameter for growing high-qualify ZnO thin films. The structural properties and surface morphologies of the thin films were characterized by the X-ray diffraction and the atomic force microscope, respectively. As for the optical properties of the films, the optical absorbance was measured in the wavelength range of 300-1100 nm by using UV-VIS spectrophotometer. The optical transmittance, absorption coefficient, and optical bandgap energy of ZnO thin films were calculated from the measured data. The crystallinity of the films was improved and the bandgap energy was increased from 3.08 eV to 3.23 eV as the oxygen flow ratio was increased from 0 % to 50 %. Furthermore, The ultraviolet and violet luminescences were observed by using photoluminescence spectroscopy. The hall mobility was decreased with the increase of oxygen flow ratio.

Effects of the Plasma Treatment on the Physical Property of ZnO Thin Film (플라즈마 처리가 ZnO 박막의 물리적 특성에 미치는 영향)

  • Cho, Jae-Won;Joung, Tae-Young;Rhee, Seuk-Joo
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.24 no.3
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    • pp.173-176
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    • 2011
  • The characteristic changes in ZnO thin film according to H- and O- plasma treatments have been studied by Photoluminescence (PL) spectroscopy at room temperature. The red shift of UV peak by 20-30 meV in PL spectra after plasma treatments is identified, which indicates that there are changes in the binding energy of bound exciton and/or the movement of energy levels of lattice defects and impurities. The width of UV peak is decreased after plasma treatments, which is believed to be closely related to the crystal quality of ZnO film. The increase of UV peak intensity after H-plasma treatment is also observed, and this could mean that the radiative recombination is strengthened because the hydrogen atoms in the plasma diffuse into the film where they passivate and neutralize the defects and the impurities.

Relation Between Defect State and Negative Ultra-Violet Photoresponse from n-ZnO/p-Si Heterojunction Diode

  • Jo, Seong-Guk;Nam, Chang-U;Kim, Eun-Gyu
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.08a
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    • pp.191.2-191.2
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    • 2013
  • The negative photoconductivity was frequently observed in some semiconductors. It was known that the origin of the negative photoresponse from ZnO is molecular chemisorption or the charging effect of nanoparticles in bulk matrix. However, the origin of the negative photoresponse of thin film was not still clear. One of possible explanation is due to the deep level trap scheme, which describes the origin of the negative photoresponse via defect state under illumination of light. However, the defect states below Fermi level have high capture rate by Coulomb effect, so that these states are usually filled by electrons if the defect states have donor-like character. Therefore the condition which the defect states located in below Fermi level should be partially filled by electrons make more difficult to understand of mechanism of the negative photoresponse. In this study, n-ZnO/p-Si heterojunction diodes were fabricated by UHV RF magnetron sputter. Then, some diodes show the negative photoresponse under ultra-violet light illumination. The defect state of the ZnO was analyzed by photoluminescence and deep level transient spectroscopy. To interpret the negative photoconductivity, band diagram was simulated by using SCAPS program.

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Fluorine-Doping Effect on Structural and Optical Properties of ZnO Nanorods Synthesized by Hydrothermal Method

  • Yoon, Hyunsik;Kim, Ikhyun;Kang, Daeho;Kim, Soaram;Kim, Jong Su;Lee, Sang-Heon;Leem, Jae-Young
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.08a
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    • pp.204.1-204.1
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    • 2013
  • Fluorine, the radius of which is close to that of oxygen, could be an appropriate anion doping candidate. A lower lattice distortion could be expected for F doping, compared with Al, Ga, and In doping. F-doped ZnO (FZO) and undoped ZnO nanorods were grown onto glass substrate by the hydrothemal method. The doping level in the solution, designated by F/Zn atomic ratio of was varied from 0.0 to 10.0 in 2.0 steps. To investigate the effects of the structure and optical properties of FZO nanorods were investigated using X-ray diffraction, UV-visible spectroscopy and photoluminescence (PL). For the PL spectra, the maximum peak position of NBE moves to higher energy, from 0 to 4 at.%. As the doping concentration increases, the maximum peak position of NBE gradually moves to lover energy, from 4 to 10 at.%.

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Influence of Sn Doping on Structural and Optical Properties of Zinc Oxide Nanorods Prepared Via Hydrothermal Process

  • Park, Hyunggil;Kim, Younggyu;Ji, Iksoo;Kim, Soaram;Kim, Jin Soo;Son, Jeong-Sik;Leem, Jae-Young
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.08a
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    • pp.203.2-203.2
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    • 2013
  • Hydrothermally grown ZnO nanorods were synthesized with various Sn contents on quartz substrates, ranging from 0 to 2.5 at% in increment 0.5 at%. Scanning electron microscopy (SEM) and ultraviolet (UV)- visible spectroscopy were used to determine the effect of Sn doping on the structural and optical properties. In the SEM images, the nanorods have hexagonal wurzite structure and the diameter of the nanorods increase with increase in the Sn contents. The optical parameters of the Sn-doped ZnO nanorods such as the absorption coefficients, optical bandgaps, Urbach energies, refractive indices, dispersion parameters, dielectric constants, and optical conductivities were gained from the transmittance and reflectance results. In the PL spectra, the NBE peaks in the UV region decrease and blue-shift with increase in the Sn contents. In addition, the DLE peaks in the visible region of the nanorods shift toward low-energy region when the ZnO nanorods doped with various Sn contents.

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