• Title/Summary/Keyword: Semiconductor doped glass

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Preparationand Characteristics of ZnS-doped Borosilicate Glass(I) (ZnS 반도체 미립자 분산 Borosilicate Glass 제조 및 물성(I))

  • 이승한;박성수;박희찬;류봉기
    • Journal of the Korean Ceramic Society
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    • v.35 no.5
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    • pp.493-498
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    • 1998
  • ZnS doped borosilicate glass for nonlinear optical application was prepared by melting and precipitation process. The optical band gap of the precipitated ZnS particles ranged from 3.83 to 3.96 eV compared with the bulk ZnS energy gap of 3.53 eV. This result was interpreted in terms of a quantum confinement effect due to small crystal size. ZnS partilcle size estimated by effective mass approximation ranged from about 39 to 83 $\AA$ It increased wtih the increase of heat tratment time and temperature.

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A Study on Properties of Ga-doped ZnO Thin Films for Annealing Temperature Change by RF Sputtering Method (RF Sputtering으로 증착한 어닐링 온도 변화에 따른 Ga-doped ZnO 박막 특성 연구)

  • Han, Seung Ik;Kim, Hong Bae
    • Journal of the Semiconductor & Display Technology
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    • v.15 no.2
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    • pp.11-15
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    • 2016
  • This paper, Ga-doped ZnO (GZO) thin films which were deposited on Corning glass substrate using an magnetron sputtering deposition technology and then the post deposition annealing process was conducted for 30 minutes at different temperature of 100, 200, 300, and $400^{\circ}C$, respectively. So as to investigate the properties for the relevant the Concentration and Oxygen Vacancy with Annealing temperature of Ga-doped ZnO thin films by RF Sputtering method. The Carrier concentration is enhanced as annealing temperature decreases, and also the oxygen vacancy concentration is enhanced as annealing temperature decreased. Oxygen vacancy will decrease along with Carrier concentration. This change in Carrier concentration is related to changes in oxygen vacancy concentration. The figure of merit obtained in this study means that Ga-doped ZnO films which annealed at $400^{\circ}C$ have the lowest Carrier concentration and Oxygen vacancy, which have the highest optoelectrical performance that it could be used as a transparent electrode.

Co-doping Effects on the Blue Up-conversion Characteristics of Fluoride Glasses (희토류 원소의 복합첨가에 의한 fluride 유리에서의 청색 상향전이현상)

  • 류선윤
    • Journal of the Korean Ceramic Society
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    • v.37 no.1
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    • pp.33-43
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    • 2000
  • Up-conversion of rare-earth element added glass is promising area for short wavelength laser source by utilizing high power semiconductor infra-red laser if the efficiency can be increased by proper method. In this study, relatively low phonon energy fluoride glasses were prepared by co-doping rare-earth elements to realize the high efficiency up-convertor. The physical, chemical, andoptical properties of co-doped fluoride glasses were measured. 10 combinations of 5 different rare-earth fluoride elements doped samples were prepared and their transition temperatures, chemical durability, density, hardness, refractive index, absorption, fluorescence, and fluorescence lifetime were measured. 480nm wavelengths blue up-conversion was found in the Yb3+/Tm3+ co-doped glass sample with 800nm laser source and the optimum composition for the most efficient blue up-conversion was found from the glass sample with 0.3 mol% TmF3 and 1 mol% YbF3.

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Sol-gel Spin-coating of ZnO Co-doped with (F, Ga) as A Transparent Conducting Thin Film ((F, Ga) 코도핑된 ZnO 투명 전도 박막의 솔-젤 제조와 특성)

  • Nam, Gil Mo;Kwon, Myoung Seok
    • Journal of the Semiconductor & Display Technology
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    • v.13 no.1
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    • pp.91-95
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    • 2014
  • (F,Ga) co-doped ZnO thin film on glass substrate was fabricated via a simple non-alkoxide sol-gel spin-coating. Contrary to the F single doped ZnO thin film, the (F,Ga) co-doped thin film showed a significant reduce in electrical resistivity after a second post-heat-treatment in reducing environment. The resulting decrease in electrical resistivity with Ga co-doping is considered to be resulted from the increases both carrier density and mobility. The optical transmittance of the (F,Ga) co-doped thin film in the visible range showed higher transmittance with Ga co-doping compared with F single doped ZnO thin film.

A Study on the Fluorine Effect of Direct Contact Process in High-Doped Boron Phosphorus Silicate Glass (BPSG)

  • Kim, Hyung-Joon;Choi, Pyungho;Kim, Kwangsoo;Choi, Byoungdeog
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.13 no.6
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    • pp.662-667
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    • 2013
  • The effect of fluorine ions, which can be reacted with boron in high-doped BPSG, is investigated on the contact sidewall wiggling profile in semiconductor process. In the semiconductor device, there are many contacts on $p^+/n^+$ source and drain region. However these types of wiggling profile is only observed at the $n^+$ contact region. As a result, we find that the type of plug implantation dopant can affect the sidewall wiggling profile of contact. By optimizing the proper fluorine gas flow rate, both the straight sidewall profile and the desired electrical characteristics can be obtained. In this paper, we propose a fundamental approach to improve the contact sidewall wiggling profile phenomena, which mostly appear in high-doped BPSG on next-generation DRAM products.

졸-겔법에 의한 CdS 분산$SiO_2$ Glass 박막의 비선형광학특성

  • 문종수;강종봉;김경문
    • Journal of the Korean Ceramic Society
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    • v.33 no.12
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    • pp.1353-1364
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    • 1996
  • Recently semiconductor doped glasses have attracted attention as nonlinear optical materials because of their large third order nonlinear optical properties. The transparent and homogeneous CdS-doped SiO2 glass thin films were obtained by the dip=coating process of the sol-gel method. Thin films were consisted of glasses containing CdS microcrystallites which were formed by dissolved Cd2+ and S2- ions in a SiO2 matrix solutions. A subsequent thermal treatment of this samples led the formation of colloidal agglomerates and finally of microcrystallites. The size of CdS microcrystallites was about 4 to 15 nm after thermal treatments at various heating conditions. From the optical absorption spectra of the CdS-doped SiO2 glass films it was found that the absorption edge was blue-shifted compared with that of the bulk CdS crystal(~2, 4 eV) and that the amount of energy shift was inversely proportional to the crystal size. And the band gap energy increased with the decrease in crystallite size indicating that the quantum size effects occured.

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Preparation and Opticaa Properties of CuCl Nanocrystallites Dispersed Nonlinear Optical Glass by Sol-Gel Process (솔-젤법에 의한 CuCl 미세결정이 분산된 비선형 광학유리의 제조 및 광특성)

  • 송석표;한원택;김병호
    • Journal of the Korean Ceramic Society
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    • v.34 no.9
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    • pp.941-948
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    • 1997
  • CuCl nanocrystallites dispersed nonlinear optical silica and borosilicate glasses were fabricated by sol-gel process. CuCl powder was dissolved in TEOS(Si(OC2H5)4) and TMB((CH3O)3B), precursors of silica and borosilicate glasses, with ethanol, water and HCl, and precipitated through the heat treatment in the matrix glass. The optical properties of CuCl doped glasses were measured using the spectrophotometer at room temperature and low temperature(77K); Z1, 2 and Z3 exciton peaks from the absorption spectra, were observed at about 370 nm and 380 nm, respectively. The average radius of nanocrystallites, calculated from the blue shift of Z3 excitons, was measured according to annealing temperature and time. The precipitation temperature of CuCl nanocrystallites was decreased when boron was added to silica glass. Increase of annealing temperature and time made average radius of nanocrystallites saturated about 2 nm.

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A Study on Properties of RF-sputtered Al-doped ZnO Thin Films Prepared with Different Ar Gas Flow Rates

  • Han, Seung Ik;Kim, Hong Bae
    • Applied Science and Convergence Technology
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    • v.25 no.6
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    • pp.145-148
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    • 2016
  • This paper, Al-doped ZnO(AZO) thin films for application as transparent conducting oxide films were deposited on the Corning glass substrate by using RF magnetron sputtering system. The effects of various Argon gas flow rates on optical and electrical characteristics of AZO films were investigate sputtering method. The Carrier Concentration is enhanced as Ar gas rate increases, and also the oxygen vacancy concentration. The figure of merit obtained in this study means that AZO films which deposited Ar gas rate of 75 sccm have the highest Carrier concentration and Hall mobility, which have the highest photoelectrical performance that it could be used as transparent electrodes.

Intensity-dependent dynamics of photoinduced absorption in CdS0.4/Se0.6 semiconductor doped glasses

  • Seo, Jung-Chul;Kim, Dong-Ho;Kong, Hong-Jin
    • Journal of the Optical Society of Korea
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    • v.1 no.1
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    • pp.15-18
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    • 1997
  • Intensity dependent dynamics of photoinduced absorption in $CdS_{0.4}$/$Se_{0.6}$ semiconductor doped glasses below the band gap was investigated by using time-resolved differential transmittance spectroscopy. The carriers populated through ultrafast trapping at semiconductor-glass interfaces give rise to a broad photoinduced absorption below the band gap. The decay time of transient absorption depends strongly on the excitation intensity. Based on our results, the physical mechanism for photoinduced absorption processes was suggested.

Preparation and Nonlinear Optical Properties of CuCl-doped Nonlinear Optical Glasses: I. Preparation, Microstructure, and Optical properties (CuCl 미립자가 분산된 비선형 광학유리의 제조와 비선형 광특성: I. 제조와 미세조직 및 광특성)

  • 윤영권;한원택
    • Journal of the Korean Ceramic Society
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    • v.34 no.4
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    • pp.420-428
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    • 1997
  • Alumino-borosilicate glasses containing nano-sized CuCl crystals for nonlinear optical application were prepared by the melting and precipitation process, and structural and optical properties were investigated by using XRD, TEM, SAXS, and optical spectroscopy. the average radius of the precipitated CuCl particles was about 2 nm. The blue shift of Z3 resonance peak with decreasing the precipitated CuCl particles size was found and the radius increased with decreasing the glass transition temperature of the matrix glass and with increasing the temperature and duration time of the precipitation heat treatment.

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