• 제목/요약/키워드: Dependence of Spectrum

검색결과 194건 처리시간 0.026초

Hot wall epitaxy방법에 의한 AgInS2 박막의 성장과 광전류 특성 (Growth and Photocurrent Properties for the AgInS2 Epilayers by Hot Wall Epitaxy)

  • 김혜숙;홍광준;정준우;방진주;김소형;정태수;박진성
    • 한국재료학회지
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    • 제12권7호
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    • pp.587-590
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    • 2002
  • A silver indium sulfide ($AgInS_2$) epilayer was grown by the hot wall epitaxy method, which has not been reported in the literature. The grown $AgInS_2$ epilayer has found to be a chalcopyrite structure and evaluated to be high quality crystal. From the photocurrent measurement in the temperature range from 30 K to 300 K, the two peaks of A and B were only observed, whereas the three peaks of A, B, and C were seen in the PC spectrum of 10 K. These peaks are ascribed to the band-to-band transition. The valence band splitting of $AgInS_2$ was investigated by means of the photocurrent measurement. The crystal field splitting, $\Delta_{cr}$ , and the spin orbit splitting, $\Delta_{so}$ , have been obtained to be 0.150 eV and 0.009 eV at 10 K, respectively. And, the energy band gap at room temperature has been determined to be 1.868 eV. Also, the temperature dependence of the energy band gap, $E_{g}$(T), was determined.d.

Hot Wall Epitaxy(HWE)법에 의한 $v_2$ 단결정 박막의 성장과 광전류 특성 (Photocurrent Properties and Growth of $CuAlSe_2$ Single Crystal Thin Film by Hot Wall Epitaxy)

  • 유상하;홍광준
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2003년도 하계학술대회 논문집 Vol.4 No.1
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    • pp.282-285
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    • 2003
  • Single crystal $CuAlSe_2$ layers were grown on thoroughly etched semi-insulating GaAs(100) substrate at $410\;^{\circ}C$ with hot wall epitaxy (HWE) system by evaporating $CuAlSe_2$ source at $680\;^{\circ}C$. The crystalline structure of the single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of single crystal $CuAlSe_2$ thin films measured with Hall effect by van der Pauw method are $9.24{\times}10^{16}\;cm^{-3}\;and\;295\;cm^2/V{\cdot}s$ at 293 K, respectively. The temperature dependence of the energy band gap of the $CuAlSe_2$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g(T)\;=\;2.8382\;eV\;-\;(8.68\;{\times}\;10^{-4}eV/K)T^2/(T\;+\;155\;K)$. The crystal field and the spin-orbit splitting energies for the valence band of the $CuAlSe_2$ have been estimated to be 0.2026 eV and 0.2165 eV at 10 K, respectively, by means of the photocurrent spectra and the Hopfield quasicubic model. These results indicate that the splitting of the $\Delta$so definitely exists in the ${\Gamma}_5$ states of the valence band of the $CuAlSe_2$. The three photocurrent peaks observed at 10 K are ascribed to the $A_1-$, $B_1-$, and $C_1$-exciton peaks for n = 1.

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Hot Wall Epitaxy(HWE)법에 의한 AgGaSe2 단결정 박막 성장과 가전자대 갈라짐에 대한 광전류 연구 (Growth and study on photocurrent of valence band splitting for AgGaSe2 single crystal thin film by hot wall epitaxy)

  • 이관교;홍광준
    • 센서학회지
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    • 제15권6호
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    • pp.397-405
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    • 2006
  • Single crystal $AgGaSe_{2}$ layers were grown on thoroughly etched semi-insulating GaAs(100) substrate at $420^{\circ}C$ with hot wall epitaxy (HWE) system by evaporating $AgGaSe_{2}$ source at $630^{\circ}C$. The crystalline structure of the single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of single crystal $AgGaSe_{2}$ thin films measured with Hall effect by van der Pauw method are $4.05{\times}10^{16}/cm^{3}$, $139cm^{2}/V{\cdot}s$ at 293 K, respectively. The temperature dependence of the energy band gap of the $AgGaSe_{2}$ obtained from the absorption spectra was well described by the Varshni's relation, $E_{g}(T)$=1.9501 eV-($8.79{\times}10^{-4}{\;}eV/K)T^{2}$/(T+250 K). The crystal field and the spin-orbit splitting energies for the valence band of the $AgGaSe_{2}$ have been estimated to be 0.3132 eV and 0.3725 eV at 10 K, respectively, by means of the photocurrent spectra and the Hopfield quasicubic model. These results indicate that the splitting of the ${\Delta}So$ definitely exists in the ${\Gamma}_{5}$ states of the valence band of the $AgGaSe_{2}$. The three photocurrent peaks observed at 10 K are ascribed to the $A_{1}-$, $B_{1}-$, and $C_{1}-$exciton peaks for n=1.

기판온도 및 열처리온도에 대한 CdS 박막의 전기적 및 광학적 특성 (Dependence of the Electrical and Optical Properties of CdS Thin Films on Substrate and Annealing Temperatures)

  • 박기철;심호섭;김정규
    • 센서학회지
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    • 제6권2호
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    • pp.163-171
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    • 1997
  • CSVT(close spaced vapor transport)증착시스템으로 태양전지의 창재에 적합한 CdS박막을 기판온도에 따라 증착하였으며, 실온에서 증착된 CdS박막을 온도를 변화시켜 가면서 열처리하였다. 증착 및 열처리후의 CdS박막의 구조적, 전기적 및 광학적 특성을 조사하였다. 증착조건에 무관하게 CdS박막들은 육방정계구조로 (002)면으로 기판에 수직으로 성장함을 확인하였다. 기판온도가 $25^{\circ}C$에서 $300^{\circ}C$까지 증가함에 따라 비저항은 $60{\Omega}cm$로 부터 $2{\times}10^{4}{\Omega}cm$로 단순증가하였으며 기판온도 $25^{\circ}C$에서 가시광영역에서의 광투과도가 80%정도로 가장 높았다. 열처리온도가 증가함에 따라 막내의 결정결함의 증가에 따라 비저항은 현저하게 증가하였으며 광투과도는 현저하게 감소하였다.

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Hot Wall Epitaxy(HWE)법에 의한 $AgGaSe_2$ 단결정 박막 성장과 광전기적 특성 (Growth and Opoelectrical property for $AgGaSe_2$ single crystal thin film by hot wall epitaxy)

  • 윤석진;홍광준
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2007년도 추계학술대회 논문집
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    • pp.122-123
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    • 2007
  • Single crystal $AgGaSe_2$ layers were grown on thoroughly etched semi-insulating GaAs(100) substrate at $420^{\circ}C$ with hot wall epitaxy (HWE) system by evaporating $AgGaSe_2$ source at $630^{\circ}C$. The temperature dependence of the energy band gap of the $AgGaSe_2$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g$(T)=1.9501 eV - $(8.79{\times}10^{-4}\;eV/K)T^2$/(T+250 K). The crystal field and the spin-orbit splitting energies for the valence band of the $AgGaSe_2$ have been estimated to be 0.3132 eV and 0.3725 eV at 10 K, respectively, by means of the photocurrent spectra and the Hopfield quasicubic model. These results indicate that the splitting of the ${\Delta}so$ definitely exists in the ${\Gamma}_5$ states of the valence band of the $AgGaSe_2$. The three photocurrent peaks observed at 10 K are ascribed to the $A_{1^-},\;B_{1^-},\;and\;C_{1^-}$exciton peaks for n=1.

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광전류 측정으로부터 얻어진 $CdGa_2Se_4$ 에피레이어의 결정장 갈라짐에 대한 에너지 (Crystal field splitting energy for $CdGa_2Se_4$ epilayers obtained by photocurrent measurement)

  • 홍광준
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2009년도 하계학술대회 논문집
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    • pp.144-145
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    • 2009
  • Single crystal $CdGa_2Se_4$ layers were grown on a thoroughly etched semi-insulating GaAs(100) substrate at $420^{\circ}C$ with the hot wall epitaxy (HWE) system by evaporating the poly crystal source of $CdGa_2Se_4$ at $630\;^{\circ}C$. The crystalline structure of the single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of single crystal $CdGa_2Se_4$ thin films measured with Hall effect by van der Pauw method are $8.27\;\times\;10^{17}\;cm^{-3}$, $345\;cm^2/V{\cdot}s$ at 293 K, respectively. The photocurrent and the absorption spectra of $CdGa_2Se_4$/SI(Semi-Insulated) GaAs(100) are measured ranging from 293 K to 10K. The temperature dependence of the energy band gap of the $CdGa_2Se_4$ obtained from the absorption spectra was well described by the Varshni's relation, $E_g$(T) = 2.6400 eV - ($7.721\;{\times}\;10^{-4}\;eV/K)T^2$/(T + 399 K). Using the photocurrent spectra and the Hopfield quasi cubic model, the crystal field energy(${\Delta}cr$) and the spin-orbit splitting energy(${\Delta}so$) for the valence band of the $CdGa_2Se_4$ have been estimated to be 106.5 meV and 418.9 meV at 10 K, respectively. The three photocurrent peaks observed at 10 K are ascribed to the $A_1$-, $B_1$-, and $C_{11}$-exciton peaks.

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고주파 마그네트론 스퍼터링법에 의해 제조된 TO:F 투명도전막의 제조 및 특성( I ) (Fabrication and Characteristics of TO:F Thin Film Deposited by RF Magnetron Sputtering( I ))

  • 박기철;김정규
    • 센서학회지
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    • 제3권2호
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    • pp.65-73
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    • 1994
  • 고주파 마그네트론 스퍼터링법에 의해 TO:F($SnO_{2}:F$)막을 제조하고 막의 구조적, 전기적 및 광학적 특성을 조사하였다. TO:F막은 $SnF_{2}$를 무게비로 첨가한 $SnO_{2}$ 타겟을 사용하여 증착되었으며 투명도전막으로서의 최적증착조건은 타겟내의 $SnF_{2}$의 첨가량이 15wt.% 고주파출력이 150W, 기판온도가 $150^{\circ}C$ 및 반응실내의 동작압력이 2mmTr일 때이다. 최적 증착조건에서 저항률은 $9{\times}10^{-4}{\Omega}{\cdot}cm$였으며 광투과도는 550nm에서 88%였다. 광투과도로부터 구해진 광학적 밴드갭은 타겟내에 $SnF_{2}$가 첨가되지 않은 경우 및 15wt.% 첨가된 경우에 각각 3.84eV 및 3.9eV로 나타났다. X-선회절분석의 결과 TO막 및 TO:F막은 (101),(200)방향으로 성장한 tetragonal rutile구조를 가지고 있었다.

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Evidence of Spin Reorientation by Mössbauer Analysis

  • Myoung, Bo Ra;Kim, Sam Jin;Kim, Chul Sung
    • Journal of Magnetics
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    • 제19권2호
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    • pp.126-129
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    • 2014
  • We report the crystallographic and magnetic properties of $Ni_{0.3}Fe_{0.7}Ga_2S_4$ by means of X-ray diffractometer (XRD), a superconducting quantum interference device (SQUID) magnetometer, and a M$\ddot{o}$ssbauer spectroscopy. In particular, $Ni_{0.3}Fe_{0.7}Ga_2S_4$ was studied by M$\ddot{o}$ssbauer analysis for evidence of spin reorientation. The chalcogenide material $Ni_{0.3}Fe_{0.7}Ga_2S_4$ was fabricated by a direct reaction method. XRD analysis confirmed that $Ni_{0.3}Fe_{0.7}Ga_2S_4$ has a 2-dimension (2-D) triangular lattice structure, with space group P-3m1. The M$\ddot{o}$ssbauer spectra of $Ni_{0.3}Fe_{0.7}Ga_2S_4$ at spectra at various temperatures from 4.2 to 300 K showed that the spectrum at 4.2 K has a severely distorted 8-line shape, as spin liquid. Electric quadrupole splitting, $E_Q$ has anomalous two-points of temperature dependence of $E_Q$ curve as freezing temperature, $T_f=11K$, and N$\acute{e}$el temperature, $T_N=26K$. This suggests that there appears to be a slowly-fluctuating "spin gel" state between $T_f$ and $T_N$, caused by non-paramagnetic spin state below $T_N$. This comes from charge re-distribution due to spin-orientation above $T_f$, and $T_N$, due to the changing $E_Q$ at various temperatures. Isomer shift value ($0.7mm/s{\leq}{\delta}{\leq}0.9mm/s$) shows that the charge states are ferrous ($Fe^{2+}$), for all temperature range. The Debye temperature for the octahedral site was found to be ${\Theta}_D=260K$.

이산시간 전압모드 CMOS 혼돈 발생회로의 특성해석 (Characteristic Analysis of the Discrete Time Voltage Mode CMOS Chaos Generative Circuit)

  • 송한정;곽계달
    • 전자공학회논문지SC
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    • 제37권3호
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    • pp.55-62
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    • 2000
  • 0.8㎛ single poly CMOS 집적회로로 구현된 이산시간 전압모드 혼돈 발생회로의 동작특성을 분석하였다. 회로내 비선형 함수 블록에 대한 선형근사식을 유도하여, 실험적으로 제작한 혼돈 발생회로의 해석이 가능하도록 하였다. 혼돈상태 판별의 주요 지표인, 입력변수에 따른 분기도를 구하였고 초기값 의존성을 보여 주는 리아프노프 지수도 계산하였다. 뿐만 아니라 상태조건, 즉 평형상태, 주기상태, 혼돈상태에 따라 나타나는 시간파형 및 상태천이관계 그리고 주파수특성을 보여주는 전력스펙트럼도 구하여 상호 연관성을 보였다. 한편 집적화 된 혼돈 발생회로를 ±2.5V 전원, 10㎑의 클럭으로 구동시켜 입력전압에 따른 분기도를 측정하였고, 상태조건에 따라 다르게 나타나는 시간파형의 측정과 이의 전력스펙트럼 분석도 실시하여 해석결과와 비교하였다.

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Comparison of the PSD radial profiles between before and after geosynchronous flux dropout: case studies using THEMIS observations

  • 황정아;이대영;김경찬;최은진;신대규;김진희;조정희
    • 천문학회보
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    • 제37권2호
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    • pp.122-122
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    • 2012
  • Geosynchronous electron flux dropouts are most likely due to fast drift loss of the particles to the magnetopause (or equivalently, the "magnetopause shadowing effect"). A possible effect related to the drift loss is the radial diffusion of PSD due to gradient of PSD set by the drift loss effect at an outer L region. This possibly implies that the drift loss can affect the flux levels even inside the trapping boundary. We recently investigated the details of such diffusion process by solving the diffusion equation with a set of initial and boundary conditions set by the drift loss. Motivated by the simulation work, we have examined observationally the energy spectrum and pitch angle distribution near trapping boundary during the geosynchronous flux dropouts. For this work, we have first identified a list of geosynchronous flux dropout events for 2007-2010 from GOES satellite electron measurements and solar wind pressures observed by ACE satellite. We have then used the electron data from the Time History of Events and Macroscale Interactions during Substorms (THEMIS) spacecraft measurements to investigate the particle fluxes. The five THEMIS spacecraft sufficiently cover the inner magnetospheric regions near the equatorial plane and thus provide us with data of much higher spatial resolution. In this paper, we report some case studies showing energy dependence during magnetopause shadowing effect.

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