• 제목/요약/키워드: excimer formation

검색결과 53건 처리시간 0.026초

Membrane-Ordering Effects of Barbiturates on Pure Phospholipid Model Membranes

  • Knag, Jung-Sook;Chung, Young-Za;Cho, Goon-Jae;Byun, Won-Tan;Yun, Il
    • Archives of Pharmacal Research
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    • 제15권3호
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    • pp.196-203
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    • 1992
  • Intramolecular excimer formation of 1, 3-di(1-pyrenyl)propane (Py-3-Py) and fluorescence polarization of 1, 6-diphenyl-1, 3, 5-hexatriene (DPH) were used to investigate the effects of barbiturates on the fluidity of model membranes of phosphatidycholine (SPMVPC), phosphatidylserine (SPMVPS), and phosphatidylinositol (SPMVPI) fractions of synaptosomal plasma membrane vesicles (SPMV) isolated from bovine cerebral cortex. In a dose-dependent manner, barbiturates decreased the excimer to monomer fluorescence intensity ratio (I'/I) of Py-3-Py and increased the anisotropy(r), rotational relaxation time (P), limiting anisotropy $(r_infty)$, and order parameter (S) of DPH in SPMVPC, SPMVPS and SPMVPI. This indicates that barbiturates decreased both the lateral and rotational diffusion of the probes in SPMVPC, SPMVPS and SPMVPI. The relative potencies of barbiturates in ordering the membranes were in the order: pentobarbital > hexobarbital > amobarbital > phenobarbital. This order correlates well with the anesthetic potencies of barbiturates and the potencies for enhancement of $\gamma$-aminobutyric acid-stimulated chloride uptake. Thus, it is strongly suggested that a close relationship might exist between the membrane ordering effects of barbiturates and the chloride fluxes across SPMV.

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Effects of Parathyroid Hormone on the Fluidity of the Plasma Membrane Vesicles of Cultured Osteoblasts

  • Kang, Jung-Sook
    • Journal of Photoscience
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    • 제8권3_4호
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    • pp.87-92
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    • 2001
  • Intramolecular excimer formation of 1,3-di(1-pyrenyl)propane (Py-3-Py) and fluorescence polarization of 1,6-diphenyl-1,3,5-hexatriene (DPH) were used to investigate the effects of parathyroid hormone (PTH) on the bulk bilayer fluidity of the plasma membrane vesicles isolated from cultured osteoblasts (OB-PMV). In a dose-dependent manner, rat PTH-(1-34) [rPTH-(1-34)] increased the excimer to monomer fluorescence intensity ratio (I'/I) of Py-3-Py and decreased the anisotropy (r) of DPH in OB-PMV. This indicates that PTH increased both the lateral and rotational diffusion of the probes in OB-PMY. Selective quenching of DPH fluorescence by trinitrophenyl groups was utilized to examine the transbilayer fluidity asymmetry of OB-PMV. The anisotropy, limiting anisotropy, and order parameter of DPH in the inner monolayer were 0.024, 0.032, and 0.062 greater than calculated for the outer monolayer of OB-PMY. Selective quenching of DPH fluorescence by trinitrophenyl groups was also utilized to examine the transbilayer effects of PTH on the fluidity of OB-PMV. rPTH-(1-34) had a greater fluidizing effect on the outer monolayer as compared to the inner monolayer of OB-PMV. Thus, it has been proven that PTH exhibits a selective rather than nonselective fluidizing effect within transbilayer domains of OB-PMV.

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Laser와 PZT - Target간의 반응과 그에 따른 Plume 형성 및 입자 방출에 관한 연구 (Interaction of Laser Beam with PZT - Target and Observation of Laser - Induced Plume and Particle Ejection)

  • 이병우
    • Journal of Advanced Marine Engineering and Technology
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    • 제20권5호
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    • pp.93-102
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    • 1996
  • Laser-induced plume and laser-target interaction during pulsed laser deposition are demonstrated for a lead zirconate titanate (PZT). A KrF excimer laser (wavelength 248nm) was used and the laser was pulsed at 20Hz, with nominal pulse width of 20ns. The laser fluence was~$16J/cm^2,$ with 100mJ per pulse. The laser-induced plasma plume for nanosecond laser irradiation on PZT target has been investigated by optical emission spectra using an optical multichannel analyzer(OMA) and by direct observation of the plume using an ICCD high speed photography. OMA analysis showed two distinct ionic species with different expansion velocities of fast or slow according to their ionization states. The ion velocity of the front surface of the developing plume was about $10^7$cm/sec and corresponding kinetic energy was about 100eV. ICCD photograph showed another kind of even slower moving particles ejected from the target. These particles considered expelled molten parts of the target. SEM morphologies of the laser irradiated targets showed drastic melting and material removal by the laser pulse, and also showed the evidence of the molten particle ejection. The physics of the plasma(plume) formation and particle ejection has been discussed.

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전자빔여기 XeF$(C\rightarrowA$ 엑시머 레이저의 출력특성에 대한 시뮬레이션 해석 (Simulation Anaysis on the Output Characteristics of XeF$(C\rightarrowA$ Excimer Laser Pumped by Electron-Beam)

  • 류한용;이주희
    • 한국광학회지
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    • 제6권3호
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    • pp.201-213
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    • 1995
  • 전자빔여기 XeF$(C\rightarrowA$ 엑시며 레이저의 상준위 B-와 C-상태에 대하여 충동혼합 운동과정을 포함하는 모델을 컴퓨터 시뮬레이션하여 이의 출력특성을 해석하였다 $XeF^*(B)$ 의 수밀도에 관련되는 $XeF^*(C)$의 형성에 대하여 레이저 에너지를 실험치와 비교하였다. 이 결과는 70ns[FWHM]의 전자빔(800kV, 21kA)을 사용한 대기압 매질에서 매우 좋은 일치$(28.5 mJ\pm5%)$를 보였고, $Xe/F_2/Ar=5.26/0.49/94.28%$의 최적화된 가스혼합비를 확인하였다. 또한 시뮬레이션으로 $XeF^*(C)$의 형성경로, $XeF^*(C)$의 완화경로, 청록색 파장대역의 흡수경로에 대한 $F_2$ 할로겐 도우너 및 Xe 압력의 함수관계를 조사하였다.

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청색발광 고분자/절연 나노층 나노 복합체의 제조 및 특성화 (Preparation and Characterization of Blue-Emitting Polymer/Dielectric Nanolayer Nanocomposites)

  • 박종혁;박오옥;김재경;유재웅;김영철
    • 한국복합재료학회:학술대회논문집
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    • 한국복합재료학회 2003년도 추계학술발표대회 논문집
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    • pp.7-10
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    • 2003
  • Blue-light-emitting peiymer/dielectric nanolayer nanocomposites were prepared by the solution intercalation method and employed in electroluminescent device. Their photoluminescence and electroluminescence characteristics suggested that the nanolayers isolate the polymer chains and hinder the formation of excimers and aggregates. By reducing the excimer formation and its deleterious effects on emission efficiency, both the color purity and the luminescence stability were improved. Furthermore, the dielectric nanolayers have an aspect ratio of about 500 and therefore act as efficient barriers to oxygen and moisture diffusion, which produced a dramatic increase in the device stability.

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방전여기 KrF 레이저의 완충가스 영향에 대한 이론 해석 (Theoretical Analysis of Buffer Gas Effects of a Discharge Excited KrF Laser)

  • 최부연;이주희
    • 한국광학회지
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    • 제1권1호
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    • pp.33-39
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    • 1990
  • 방전여기 방식의 KrF 엑사이머 레이저의 컴퓨터 시뮬레이션 프로그램을 개발하여 방전 중의 $KrF^*$ 형성, 탈여기 및 흡수반응 등에 대한 완충가스의 영향에 관해 해석하였다. He 가스와 Ne 가스의 경우 $KrF^*$ 생성효율은 각각 7.5%, 19%였으며, $KrF^*$ 탈여기는 충전전압 30kV에서 각각 45, 30%의 비율을 차지하였다. 그러나 흡수과정에서는 완충가스의 영향이 10% 이하였다.

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형광분석기를 이용한 에폭시-산무수물계의 경화 모니터링 (Cure Monitoring of Am Epoxy-Anhydride System by Means of Fluorescence Spectroscopy)

  • 조동환;김득수;이종근
    • 폴리머
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    • 제25권2호
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    • pp.199-207
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    • 2001
  • 본 연구에서는 경화촉진제로서 N,N-dimethyl benzyl amine (BDMA) 또는 1-cyanoethyl-2-ethyl-4-methyl imidazole (2E4MZ-CN)을 포함하고 있는 산무수물계 경화제에 의한 diglycidyl ether of bisphenol-A (DGEBA)의 경화거동을 형광분석기를 사용하여 광물리적 특성 변화의 관점에서 해석하였다. 이를 위해 1,3-bis-(1-pyrene)propane (BPP) probe를 에폭시수지 내에 균일하게 도입시켰다. 주위 환경 겔화에 의한 분자의 공간구조 변화에 민감한 BPP probe는 분자내 여기체 형광을 잘 형성하였으며 에폭시수지의 경화반응에 따른 미세점도 변화 또는 분자의 움직임에 민감하였다. 에폭시수지의 경화거동은 경화시간, 경화온도 및 경화촉진제의 종류에 따른 단량체 형광세기 ($I_{M}$ ), 여기체 형광세기 ($I_{E}$ ) 그리고 $I_{M}$ /$I_{E}$ 값의 변화로부터 설명되었다. 그 결과는 이전의 DSC 또는 torsion pendulum을 이용하여 에폭시-산무수물계에 대하여 얻어진 경화거동 결과와 일치하였다. 또한, 형광분석 방법은 다른 분석 방법에서 해석이 어려운 저온영역에서의 열경화성 수지의 경화거동에 대한 정보를 제시하였다.

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Excimer-Based White Phosphorescent OLEDs with High Efficiency

  • Yang, Xiaohui;Wang, Zixing;Madakuni, Sijesh;Li, Jian;Jabbour, Ghassan E.
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2008년도 International Meeting on Information Display
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    • pp.1520-1521
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    • 2008
  • There are several ways to demonstrate white organic light emitting diodes (OLEDs) for displays and solid state lighting applications. Among these approaches are the stacked three primary or two complementary colors light-emitting layers, multiple-doped emissive layer, and excimer and exciplex emission [1-10]. We report on white phosphorescent excimer devices by using two light emitting materials based on platinum complexes. These devices showed a peak EQE of 15.7%, with an EQE of 14.5% (17 lm/W) at $500\;cd/m^2$, and a noticeable improvement in both the CIE coordinates (0.381, 0.401) and CRI (81). Devices with the structure ITO/PEDOT:PSS/TCTA (30 nm)/26 mCPy: 12% FPt (10 nm) /26 mCPy: 2% Pt-4 (15 nm)/BCP (40 nm)/CsF/Al [device 1], ITO/PEDOT:PSS/TCTA (30 nm)/26 mCPy: 2% Pt-4 (15 nm)/26 mCPy: 12% FPt (10 nm)/BCP (40 nm)/CsF/Al [device 2], and ITO/PEDOT:PSS/TCTA (30 nm)/26 mCPy: 2% Pt-4: 12% FPt (25 nm)/BCP (40 nm)/CsF/Al [device 3] were fabricated. In these cases, the emissive layer was either the double-layer of 26 mCPy:12% FPt and 15 nm 26 mCPy: 2% Pt-4, or the single layer of 26mCPy with simultaneous doping of Pt-4 and FPt. Device characterization indicates that the CIE coordinates/CRI of device 2 were (0.341, 0.394)/75, (0.295, 0.365)/70 at 5 V and 7 V, respectively. Significant change in EL spectra with the drive voltage was observed for device 2 indicating a shift in the carrier recombination zone, while relatively stable EL spectra was observed for device 1. This indicates a better charge trapping in Pt-4 doped layers [10]. On the other hand, device 3 having a single light-emitting layer (doped simultaneously) emitted a board spectrum combining emission from the Pt-4 monomer and FPt excimer. Moreover, excellent color stability independent of the drive voltage was observed in this case. The CIE coordinates/CRI at 4 V ($40\;cd/m^2$) and 7 V ($7100\;cd/m^2$) were (0.441, 0.421)/83 and (0.440, 0.427)/81, respectively. A balance in the EL spectra can be further obtained by lowering the doping ratio of FPt. In this regard, devices with FPt concentration of 8% (denoted as device 4) were fabricated and characterized. A shift in the CIE coordinates of device 4 from (0.441, 0.421) to (0.382, 0.401) was observed due to an increase in the emission intensity ratio of Pt-4 monomer to FPt excimer. It is worth noting that the CRI values remained above 80 for such device structure. Moreover, a noticeable stability in the EL spectra with respect to changing bias voltage was measured indicating a uniform region for exciton formation. A summary of device characteristics for all cases discussed above is shown in table 1. The forward light output in each case is approximately $500\;cd/m^2$. Other parameters listed are driving voltage (Bias), current density (J), external quantum efficiency (EQE), power efficiency (P.E.), luminous efficiency (cd/A), and CIE coordinates. To conclude, a highly efficient white phosphorescent excimer-based OLEDs made with two light-emitting platinum complexes and having a simple structure showed improved EL characteristics and color properties. The EQE of these devices at $500\;cd/m^2$ is 14.5% with a corresponding power efficiency of 17 lm/W, CIE coordinates of (0.382, 0.401), and CRI of 81.

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$0.1{\mu}m$급 dense 패턴 형성을 위한 사입사 조명 조건과 OPC 보조 패턴 크기의 최적 조건에 관한 연구 (Research on the optimization of off-axis illumination condition and sub-resolution pattern size for the $0.1{\mu}m$ rule dense pattern formation)

  • 박정보;이재봉;이성묵
    • 한국광학회지
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    • 제12권3호
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    • pp.190-199
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    • 2001
  • 본 연구에서는 193nm의 ArF excimer laser 광원과 0.65의 NA를 갖는 광학계에서 기본 선폭이 $0.1{\mu}m$이고 duty ratio 가 1:1인 dense line & space(LS) 패턴에 대하여 여러사입사 조명 조건에 따른 초점심도(Depth of Focus; DOF)와 cutoff intensity를 확인하고 기본 capacitor 패턴에서 광학적 근접효과 보정을 위한 hammer head형 보조 패턴의 크기와 여러사입사 조건에 다른 DOF와 cutoff intensity의 변화에 대하여 알아보았다. 그결과 0.1$\mu$m급의 dense 패턴 구현을 위해서는 전형적인 X자형 사구 조명보다는 십자(+)형 사구 조명이나 환형조명이 보다 효과적인 것을 알수 있었다. 이와 더불어 보조 패턴의 크기가 약간 변한다 하더라도 일정한 초점심도와 cutoff intensity를 유지하는 경향을 보이는 특정한 조명 조건이 존재함을 밝히고 그에 따라 최적의 조명 조건과 보조 패턴의 크기에 대하여 알아보았다.

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횡방향 전자빔여기 XeCl 엑시머 레이저의 출력특성 (Output Ccharacteristics of XeCl Excimer Laser Excited by Transeverse-Electron-Beam)

  • 류한용;이주희;김용평
    • 한국광학회지
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    • 제5권3호
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    • pp.386-393
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    • 1994
  • XeCl 엑시머 레이저를 횡방향의 전자빔으로 여기하여 이의 출력특성을 조사하였다. 전자빔의 출력은 880kV, 21kA(70ns, FWHM)이며 전자빔의 전류밀도는 다이오드(A-K) 간격과 공진기 외부에 설치한 펄스자계코일(4.7kG)로 제어하였다. 레이저 매질에 주입되는 전자빔의 축적에너지는 35J(4기압)이다. 축적에너지는 Radcolor film의 감광면적과 압력상승법에 의해 측정한 가스매질의 상승압력으로부터 환산된 수치이며, 이 때의 여기체적은 $320cm^{3}$이었다. 레이저 가스의 혼합비율은 HCl/Xe/Ar=0.2/6.3/93.5%이고 총압력이 3기압일 때, 최대효율 1.7%를 얻었다. 이 때의 출력에너지, 특성에너지는 각각 0.52J, 1.7J/l이었다. 실험결과의 분석을 위해 컴퓨터 시뮬레이션코드를 완성하였다. 시뮬레이션 결과는 실험결과와 잘 부합하고 있음을 확인하였고 그 결과를 이용하여 XeCl의 형성채널, 완화채널, 308nm의 흡수채널을 이론적으로 설명하였다.

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