• Proceedings of the Materials Research Society of Korea Conference
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• 1994.11a
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• pp.97-97
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• 1994

Wide gap 반도체 중 하나인 GaN 에너지갭이 실온에서 3.4eV 이고 직접천이형 에너지대 구조를 가지므로 청색 및 자외영역의 파장을 발광하는 발광다이오드와 바도체 레이저 다이오드의 제작에유용한 재료이다. GaN계 III족 질화물반도체가 다파장용 광원으로서 유망함을 보인 것은 1970년대 초방의기초적 연구이다. 이로부터 약 25년이 경고한 현재 청색발광다이오드가 실용화당계에 이르게 되었지만 아직까지 전류주입에 의한 레이저발진은 보고되고있지 않다. 이 논문에서는 ALGaN/GaN이중이종접합(DH) 구조의 광여기에 의한 유도방출과 광학적 이득을 측정하므로서 전류주입에의한 레이저발진의 가능성을 조사하였다. 유기금속기상에피텍셜(MOVPE)법으로 성장한 ALGaN/GaN DH구조의 표면에 수직으로 펄스발진 질소레이저(파장:337.1nm, 주기:10Hz, 폭: 8nsec) 빔의 공출력밀도를 변화시키어 조사하고 시료의단면 혹은 표면으로부터 방출되는 광 스펙트럼을 측정하였다. 입상광밀도가 증가함에 따라 자연방출에 의한 발광피크보다 낮은 에너지에서 발광강도가 큰 유도방출에 의한 피크가 370nm의 파장에서 현저하게 나타났으며 실온에서 유동방출에 필요한 입사공밀도의 임계치는 약 89㎾/$\textrm{cm}^2$이었다. 이는 GaN 단독층에 대한 유동방출의 임계치 700㎾/$\textrm{cm}^2$ 에 비하여 약 1/8정도 낮은 것이며, 이를 전류밀도로 환산하면 약 27㎄/$\textrm{cm}^2$ 정도로서 전류주입에 의하여서도 레이저발진을 실현할 수 있는 현실적인 값이다. 한편 광여기 방법으로 측정한 광학적 이득은 입사광의 밀도가 각각 100㎾/$\textrm{cm}^2$과 200㎾/$\textrm{cm}^2$일 때 34$cm^{-1}$ / 과 160 $cm^{-1}$ / 이었다. 이와 같은 결과는 GaN의밴드단 부근의 파장영역에서 AIGaN 흔정의 굴절율이 GaN의 굴절율보다 작으므로 DH구조의 채택의 의한 광의 몰입이 가능하여 임계치가 저하된 것으로 여겨진다. 또한 광학적 이득의 존재는 이 구조에 의한 극단파장 반도체 레이저다이오드의 실현 가능성을 나타내는 것이다.

• Transactions of the Korean Society of Mechanical Engineers
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• v.10 no.2
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• pp.198-207
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• 1986

This study investigates interlaminar fracture characteristics of Graphite/Epoxy composite (HFG Graphite/Epoxy) under mode I (opening mode), mode II (sliding mode) and mixed mode loading conditions. The effects on interlaminar fracture toughness due to different fiber orientations on the crack surface are also investigated. The antisymmetric test fixture proposed by M. Arcan is used for this test. Both critical stress intensity foctors and critical energy release rates were determined and several mixed mode fracture criteria were compared to the experimental data. Also fracture surfaces were investigaed to obtain informations on the fracture behaviors of Graphite/Epoxy composite by means of a scanning electron microscope(SEM).

• Journal of the Korean Institute of Telematics and Electronics D
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• v.35D no.12
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• pp.59-67
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• 1998

In this paper, a rigorous three-dimensional Monte Carlo approach to simulate the sputter yield as a function of the incident ion energy and the incident angle as well as the atomic ejection distribution of the target is presented. The sputter yield of the target atom (Cu, Al) has been calculated for the different species of the incident atoms with the incident energy range of 10 eV ~ 100 KeV, which coincides with the previously reported experimental results. According to the simulation results, the calculated sputter yield tends to increase with the amount of the energy of the incident atoms. Our simulation revealed that the maximum sputter yield can be obtained for the incident atom with 10 KeV for the heavy ion, while the maximum sputter yield for the light ion is for the incident atoms with an energy less than 1 KeV. The sputter yield increases with angle of incidence and seems to have the maximum value at 68$^{\circ}$. For angular distributions of the sputtered particle, the atoms in the direction normal to the surface increase with angle of incidence. Furthermore, we has conducted the parallel computation on CRAY T3E supercomputer and built a GUI(Graphic User Interface) system running the sputter simulator.

• Elastomers and Composites
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• v.39 no.1
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• pp.42-50
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• 2004

In this work, the diglycidylether of bisphenol A (DGEBA) and modified polyurethane (PU) blends were initiated by N-benzylpyrazinium hexafluoroantimonate (BPH). The cure and fracture toughness of neat DGEBA with the addition of PU were investigated. The cure properties of DGEBA/PU blend system were examined by DSC and near-IR measurements. The fracture touhtness were investigated by measuring the critical stress intensity factor ($K_{IC}$) and the critical strain energy release rate ($G_{IC}$). According to the results, the maximum values of owe activation energy ($E_a$) and conversion (${\alpha}$) were found at 10 phr of PU. Also the $K_{IC}$ showed a similar behavior with the results of conversion. These results were probably due to increase of crosslinking density in the blends resulted from increase of the hydrogen bonding between the hydroxyl groups of DGEBA and isocyanate groups of PU.

• Journal of the Korean Chemical Society
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• v.37 no.11
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• pp.961-966
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• 1993

The determination of noble metals such as Ir, Au and Ag in the ancient coins has been studied. For the measurement of the activity of $^{192}Ir,\;^{198}Au\;and\;^{110m}Ag$, radiochemical separations including solvent extraction and ion-exchange chromatography were applied to reduce the interference of high energy ${\gamma}$-ray emitted from various radionuclides with long half-life. As a results, $10^{-11}$ g/g level of Ir could be detected and it was found that the three kinds of the detection limits, i.e., critical, detection, quantitative limit, calculated by the method proposed by Currie, were enhanced. Prior to the re-irradiation with neutron, inactive carrier was added in order to determine the recovery yield of Ir in the radiochemical separation. The average recovery yields of Ir, Au and Ag in the 5 coins were 65.3%, 98.5%, 99.5%, respectively.

• Journal of the Korean Society of Hazard Mitigation
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• v.10 no.6
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• pp.59-64
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• 2010

Building a firebreak against surface forest fire is a typical indirect suppression method that stops spread of flame by removing surface fuel, such as fallen leaves and bushes. In the sense of fire dynamic, building a firebreak is to set a section which will block thermal energy from igniting on virgin fuel. This study suggests and evaluates a calculation method for width of firebreak against surface fire for variant wind and slope conditions by applying the Point Source Model (PSM) to fallen leaves of Pinus densiflora. Width of firebreak was measured based on the distance the threshold radiant heat igniting Pinus densiflora fallen leaves at the heat flux of $4.9\;kW/m^2$ reaches. As a result, at the wind velocity of 0~5 m/s and on the slope of $0{\sim}50^{\circ}$, the appropriate width of a firebreak was 0.35~0.65 m for the mean flame height and 0.75~1.05 m for the maximum flame height. Accordingly, considering the factor of safety, the most appropriate width of a firebreak is 1.05 m based on the maximum flame height. Additional comparative analyses through experiments and field surveys are deemed necessary to determine appropriate widths of firebreak for different types of surface fuel.