• 제목/요약/키워드: $As_{40}Ge_{10}Se_{15}S_{35}$ single-layer

검색결과 5건 처리시간 0.022초

DPSS Laser에 의한 As40Ge10Se15S35, Ag/As40Ge10Se15S35와 As40Ge10Se15S35/Ag/As40/Ge10Se15S35박막의 홀로그래픽 데이터 격자형성 (Holographic Data Grating Formation of As40Ge10Se15S35 Single Layer, Ag/As40Ge10Se15S35 Double Layer and As40Ge10Se15S35/Ag/As40/Ge10Se15S35 Multi-layer Thin Films with the DPSS Laser)

  • 구용운;정홍배
    • 한국전기전자재료학회논문지
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    • 제20권3호
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    • pp.240-244
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    • 2007
  • We investigated the diffraction grating efficiency by the Diode Pumped Solid State(DPSS 532 nm) laser beam wavelength to improve the diffraction efficiency on $As_{40}Ge_{10}Se_{15}S_{35},\;Ag/As_{40}Ge_{10}Se_{15}S_{35}$ and $As_{40}Ge_{10}Se_{15}S_{35}/Ag/As_{40}Ge_{10}Se_{15}S_{35}$ thin film. Diffraction efficiency was obtained from DPSS laser, used (P:P)polarized laser beam on each thin films. As a result, for the laser beam intensity in $0.24mW/cm^2$, single $As_{40}Ge_{10}Se_{15}S_{35}$ thin film shows the highest value of 0.161% diffraction efficiency at 300 s and for laser beam intensity in $2.4mW/cm^2$, it was recorded with the fastest speed of 50 s(0.013%), which the diffraction grating forming speed is faster than that of $0.24mW/cm^2$ beam. $Ag/As_{40}Ge_{10}Se_{15}S_{35}$ double layer and $As_{40}Ge_{10}Se_{15}S_{35}/Ag/As_{40}Ge_{10}Se_{15}S_{35}$ multi-layered thin film also show the faster grating forming speed at $2.4mW/cm^2$ and higher value of diffraction efficiency at $0.24mW/cm^2$.

$MgF_{2}/As_{40}Ge_{10}Se_{15}S_{35}$ 다층박막에서 편광상태에 따른 회절효율 특성 (Characteristics of the Polarization Dependence Holographic Diffraction Efficiency using the $MgF_{2}/As_{40}Ge_{10}Se_{15}S_{35}$ Multi-Layer)

  • 이정태;여철호;신경;이기남;김종빈;정홍배
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2003년도 춘계학술대회 논문집 디스플레이 광소자분야
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    • pp.127-130
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    • 2003
  • We have carried out two-beam interference experiment to form holographic grating on amorphous $As_{40}Ge_{10}Se_{15}S_{35}$ single-laver, $MgF_{2}/As_{40}Ge_{10}Se_{15}S_{35}$ muliti-layer. In this study holographic grating formed using He-Ne laser(632.8nm) under different polarization state(intensity, phase polarization holography). The diffraction efficiency was obtained by first order intensity. The maximum diffraction efficiency of $As_{40}Ge_{10}Se_{15}S_{35}$ single-laver was 0.8% and The maximum diffraction efficiency of $MgF_{2}/As_{40}Ge_{10}Se_{15}S_{35}$ multi-layer(multi-layer I, multi-layer II) were 1.4% and 3.1%.

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Ag 및 MgF2/AsGeSeS 다층박막에서의 편광 홀로그래피 회절효율 특성 (The Properties of Diffraction Efficiency in Polarization Holography using the Ag and MgF2/AsGeSeS Multi-layer)

  • 나선웅;여철호;정홍배;김종빈
    • 한국전기전자재료학회논문지
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    • 제15권12호
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    • pp.1070-1074
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    • 2002
  • We have carried out two-beam interference experiments to form holographic gratings on As$_{40}$ Se$_{15}$ S$_{35}$Ge$_{10}$ single layer, Ag/As$_{40}$ Se$_{15}$ S$_{35}$Ge$_{10}$ multi-layer. In this study, holographic gratings have been formed using He-Ne laser(632.8nm) under different polarization combinations(intensity polarization holography, phase polarization holography). The diffraction efficiency was obtained by the +lst order intensity. The maximum diffraction efficiency of As$_{40}$ Se$_{15}$ S$_{35}$Ge$_{10}$ single layer, As$_{40}$ Se$_{15}$ S$_{35}$Ge$_{10}$ and MgF$_2$/As$_{40}$ Se$_{15}$ S$_{35}$Ge$_{10}$ multi-layer were 0.8%, 1.4% and 3.1% under intensity polarization holography, respectively.

Ag가 도핑된 칼코게나이드 $As_{40}Ge_{10}Se_{15}S_{35}$ 박막의 광분해, 광확산특성 및 홀로그래픽 격자형성 (Photodissolution, photodiffusion characteristics and holographic grating formation on Ag-doped $As_{40}Ge_{10}Se_{15}S_{35}$ chalcogenide thin film)

  • 정홍배
    • 대한전기학회논문지:전기물성ㆍ응용부문C
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    • 제55권10호
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    • pp.461-466
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    • 2006
  • In the present work, we investigated the photodissolution and photodiffusion effect on the interface of Ag/chalcogenide $As_{40}Ge_{10}Se_{15}S_{35}$ thin film by measuring the absorption coefficient, the optical density, the resistance change of Ag layer. It was found that the photodissolutioniphotodiffution ratio depends on the magnitude of photon energy absorbed in the chalcogenide thin film and the depth of photodiffution was proportional to the square root of the exposed time. Also, we have investigated the holographic grating formation with P-polarization states on chalcogenide $As_{40}Ge_{10}Se_{15}S_{35}$ thin film and $As_{40}Ge_{10}Se_{15}S_{35}/Ag$ double layer structure thin film. Holographic gratings have been formed using He-Ne laser (632.8 nm) which have a smaller energy than the optical energy gap, $E_g\;_{opt}$ of the film, i. e., an exposure of sub-bandgap light $(h{\upsilon} under P-polarization. As the results, we found that the diffraction efficiency on $As_{40}Ge_{10}Se_{15}S_{35}/Ag$ double layer structure thin film was more higher than that on single $As_{40}Ge_{10}Se_{15}S_{35}$ thin film. Also, we obtained that the maximum diffraction efficiency was 0.27 %, 1,000 sec on $As_{40}Ge_{10}Se_{15}S_{35}\;(1{\mu}m)/Ag$ (10 nm) double layer structure thin film by (P: P) polarized recording beam. It will offer lots of information for the photodoping mechanism and the analyses of chalcogenide thin films.

두께에 따른 비정질 칼코게나이드 $Ag/As_{40}Ge_{10}Se_{15}S_{35}$ 박막의 홀로그래피 데이터 격자형성 (The Formation of Holographic Data Grating on Amorphous Chalcogenide $Ag/As_{40}Ge_{10}Se_{15}S_{35}$ Thin Films with Various Thickness)

  • 여철호;정홍배
    • 대한전기학회논문지:전기물성ㆍ응용부문C
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    • 제55권8호
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    • pp.387-391
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    • 2006
  • The Ag photodoping effect in amorphous $As_{40}Ge_{10}Se_{15}S_{35}$ chalcogenide thin films for holographic recording has been investigated using a He-Ne laser (${\lambda}$=632.8 nm). The chalcogenide films thickness prepared in the present work were thinner in comparison with the penetration depth of recording light ($d_p=1.66{\mu}m$). It exhibits a tendency of the variation of the diffraction efficiency (${\eta}$) in amorphous chalcogende films, independently of the Ag photodoping. That is, ${\eta}$ increases rapidly at the beginning of the recording process and reaches the maximum (${\eta}_{max}$) and slowly decreases slowly with the exposed time. In addition, the value of ${\eta}_{max}$ depends strongly on chalcogenide film thickness(d) and its maximum peak among the films with d = 40, 80, 150, 300, and 633 nm is observed 0.083% at d = 150 nm (approximately 1/2 ${\Delta}n$), where ${\Delta}$n is the refractive index of chalcogenide thin film (${\Delta}n=2.0$). The ${\eta}$ is largely enhanced by Ag photodoping into the chakogenides. In particular, the value of ${\eta}_{max}$ in a bilayer of 10-nm-thick Ag/150-nm-thick $As_{40}Ge_{10}Se_{15}S_{35}$ film is about 1.6%, which corresponds to ${\sim}20$ times larger than that of the single-layer $As_{40}Ge_{10}Se_{15}S_{35}$ thin film (without Ag). And we obtained the diffraction pattern according to the formation of (P:P) polarization holographic grating using Mask pattern and SLM.