• Proceedings of the Korean Vacuum Society Conference
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• 2011.08a
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• pp.300-300
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• 2011

알루미늄을 이용한 배선은 반도체 소자가 초집적화와 초소고속화 됨에 따라, 피로현상과 지연시간 등 배선으로서의 많은 문제점을 가지고 있어, 차세대 배선 재료로서 전기적인 특성 등이 우수한 구리에 대한 연구가 많이 진행되고 있다. 하지만, 구리는 낮은 온도에서 확산이 잘되어 배선 층간의 절연에 문제점을 야기 시킨다. 따라서, 구리를 배선에 적용하여 신뢰성 있는 제품을 만들기 위해서는 확산방지막이 필요하다. 확산방지막은 집적화와 더불어 배선의 두께가 줄어 듦에 따라 소자의 특성에 영향을 미치지 않는 범위 내에서 저항은 낮고, 두께는 얇아야 하며, 높은 종횡비를 갖는 구조에서도 균일한 박막을 형성하여야 하므로, 원자층 증착공정을 이용한 연구가 주를 이루고 있다. 텅스텐 질화막을 이용한 확산방지막은 WF6 전구체를 이용한 보고가 많지만, 높은 증착 온도와 부산물로 인한 부식가능성 이라는 문제점을 안고 있다. 따라서 본 연구에서는, 기존의 할라이드 계열을 이용한 원자층 증착공정의 단점을 보완하기 위하여, 아마이드 계열의 전구체를 사용하여 텅스텐 질화막을 형성하였으며, 이를 통해 공정온도를 낮출 수 있었다.

• Korean Journal of Materials Research
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• v.7 no.12
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• pp.1052-1057
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• 1997

현재 전기, 전자, 우주, 자동차, 무기 등의 여러 분야에서 응용되고 있는 TaNx 다층박막저항체의 특성을 개선하기 위하여 magnetron sputtering법으로 TaNx박막을 제조한 후, 온도와 질소분압에 따른 전기저항 및 TCR특성 변화를 조사하였고, 미세조직이 이들 전기적 성질에 미치는 영향을알아보기 위해 상분석과 morphology를 관찰하였다. 그 결과, TaNx을 코팅한 박막의 전기저항은 $N_{2}$Ar이 0.4 이상에서, 금속전도특성에서 이온전도특성으로 변화하였으며,Cr이 TCR효과를 안정시키는 역할은 하여 TaNx/A $I_{2}$ $O_{3}$보다 TaNx/Cr/A $i_{2}$ $O_{3}$박막의 TCR특성이 더 안정하게 나타났다. 또한 TaNx/A $I_{2}$ $O_{3}$박막과 TaNx/Cr/A $i_{2}$ $O_{3}$박막의 경우 모두 $N_{2}$/Ar이 0-0.4정도에서 TCR효과에 좋은 특성을 나타내었다. X-선회절 실험 결과 $N_{2}$/Ar비가 1일 경우에 T $a_{2}$ $N_{.8}$이 생성되었고, 분압이 증가함에 따라 비정질이 생성되었다. morphology가 $N_{2}$/Ar이 증가함에 따라 입자의 모양이 불연속아일랜드 형태로 변화하였으며, 이것은 질소분압에 따른 전기저항 변화와 일치하였다.다.

• Korean Journal of Materials Research
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• v.16 no.8
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• pp.473-478
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• 2006

The coherent interface energies and misfit strain energies of Fe/XN (X=Ti, Zr, Hf) systems were calculated by first principles method. The interface energies in Fe/TiN, Fe/ZrN and Fe/HfN systems were 0.343, 0.114, and 0.030 $J/m^2$, respectively. Influence of bond energy was estimated using the discrete lattice plane/nearest neighbor broken bond(DLP/NNBB) model. It was found that the dependence of interface energy on the type of nitride was closely related to changes of the bond energies between Fe, X and N atoms before and after formation of the Fe/XN interfaces. The misfit strain energies in Fe/TiN, Fe/ZrN, and Fe/HfN systems were 0.239, 1.229, and 0.955 eV per 16 atoms(Fe; 8 atoms and XN; 8 atoms). More misfit strain energy was generated as the difference of lattice parameters between the bulk Fe and the bulk XNs increased.

• Korean Journal of Materials Research
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• v.12 no.3
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• pp.190-194
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• 2002

InN/GaN multi-layers were grown by metalorganic chemical vapor deposition(MOCVD) in order to get the appropriate structure for an high power blue-green light emitting diode(LED), and effects of growth conditions (growth temperature, pressure, and $trimethylindium(TMIn)-NH_3-N_2\; flow\; rare)$ on the integrated photoluminescence (PL) intensity and PL peak energy in InN/GaN multi-layers were investigated. The optimized growth conditions with the highest integrated PL intensity for InN/GaN multi-layers were obtained: the growth temperature at $780^{\circ}C$, the growth pressure at 325 Torr, the TMIn flow rate with 150 $m\ell$/min, the $NH_3$flow rate with 3.2 ι/min, and $N_2$ flow rate with 2 ι/min.

• Korean Journal of Materials Research
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• v.19 no.8
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• pp.417-420
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• 2009

This study develops a highly transparent ohmic contact using phosphorus doped ZnO with current spreading for p-GaN to increase the optical output power of nitride-based light-emitting diodes (LEDs). The phosphorus doped ZnO transparent ohmic contact layer was prepared by radio frequency magnetron sputtering with post-deposition annealing. The transmittance of the phosphorus doped ZnO exceeds 90% in the region of 440 nm to 500 nm. The specific contact resistance of the phosphorus doped ZnO on p-GaN was determined to be $7.82{\times}10^{-3}{\Omega}{\cdot}cm^2$ after annealing at $700^{\circ}C$. GaN LED chips with dimensions of $300\times300{\mu}m$ fabricated with the phosphorus doped ZnO transparent ohmic contact were developed and produced a 2.7 V increase in forward voltage under a nominal forward current of 20 mA compared to GaN LED with Ni/Au Ohmic contact. However, the output power increased by 25% at the injection current of 20 mA compared to GaN LED with the Ni/Au contact scheme.

• Korean Journal of Materials Research
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• v.19 no.8
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• pp.443-446
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• 2009

This study develops a highly transparent ohmic contact scheme using indium oxide doped ZnO (IZO) as a current spreading layer for p-GaN in order to increase the optical output power of nitride-based lightemitting diodes (LEDs). IZO based contact layers of IZO, Ni/IZO, and NiO/IZO were prepared by e-beam evaporation, followed by a post-deposition annealing. The transmittances of the IZO based contact layers were in excess of 80% throughout the visible region of the spectrum. Specific contact resistances of $3.4\times10^{-4}$, $1.2\times10^{-4}$, $9.2\times0^{-5}$, and $3.6\times10^{-5}{\Omega}{\cdot}cm^2$ for IZO, Ni/Au, Ni/IZO, and NiO/IZO, respectively were obtained. The forward voltage and the optical output power of GaN LED with a NiO/IZO ohmic contact was 0.15 V lower and was increased by 38.9%, respectively, at a forward current of 20 mA compared to that of a standard GaN LED with an Ni/Au ohmic contact due to its high transparency, low contact resistance, and uniform current spreading.

• Transactions of the Korean Society of Mechanical Engineers A
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• v.30 no.10 s.253
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• pp.1314-1319
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• 2006

This paper describes the novel fabrication method of the high-aspect-ratio nano structure which is impossible by conventional method using a shadow mask and a Deep X-ray Lithography (DXRL). The shadow mask with $1{\mu}m-sized$ apertures is fabricated on the silicon membrane using a conventional UV-lithography. The size of aperture is reduced to 200nm by accumulated low stress silicon nitride using a LPCVD (low pressure chemical vapor deposition) process. The X-ray mask is fabricated by depositing absorber layer (Au, $3{\mu}m$) on the back side of nano shadow mask. The thickness of an absorber layer must deposit dozens micrometers to obtain contrast more than 100 for a conventional DXRL process. The thickness of $3{\mu}m-absorber$ layer can get sufficient contrast using a central beam stop method, blocking high energy X-rays. The nano circle and nano line, 200nm in diameter in width, respectively, were demonstrated 700nm in height with a negative photoresist of SU-8.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.02a
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• pp.252-252
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• 2013

최근 그래핀, hexagonal boron nitride (h-BN) 및 $MoS_2$ (molybdenum disulfide)와 같은 2차원 결정 물질들은 무어의 법칙(Moore's Law)를 뛰어넘어 계속적인 소자의 소형화를 가능케 하고 또한 대면적, 저비용 소자 개발을 가능케 하는 우수한 특성을 가진 차세대 반도체 트랜지스터 소재로 각광받고 있다. $MoS_2$는 bulk 상태일 때는 1.2 eV의 indirect 밴드갭을 가지지만 단층형태일 때는 1.8 eV의 direct 밴드갭을 가지며 dielectric screening 기법등을 통해 mobility를 향상시킬 수 있는 것으로 연구된 바 있다. 본 연구에서는 화학기상증착 (chemical vapor deposition)법을 이용하여 $MoS_2$ 박막을 형성하기 위한 기초연구인 Mo 전구체의 특성평가 및 적합한 공정조건 개발 연구를 수행하였다. 사용한 전구체는 $Mo(CO)_6$ (Molybdenum hexacarbonyl)이고, 온도 및 압력, 반응기체(H2 S, Hydrogen sulfide) 유량 등의 공정 조건 변화에 따른 거동을 Fourier transform infrared spectroscopy (FT-IR) 시스템을 사용하여 측정하였다. 또한 $Mo(CO)_6$의 분자구조를 상용 프로그램인 Gaussian으로 시뮬레이션 하여 실제 FT-IR 측정 결과값과 비교 분석하였다.

• Proceedings of the KIEE Conference
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• 1994.07b
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• pp.1333-1335
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• 1994

The nitrification of pure iron powders is found to occur even at room temperature by high energy ball milling in $NH_3$ gas atmosphere. The powders of metastable iron nitrides ($0<at.%N{\le}23.3$) thus produced are identified as the super-saturated bee structure for the N content below 14.9 at.%N and the high temperature phase of the hcp structure above 19.4 at.%N. The atomic volume of Fe in the bcc phase is found to be smaller than that of the N-martensite reported in the literature. Magnetization at room temperature gradually decreases with increasing the N concentration in contrast to the enhancement reported for the bet nitrides. Neutron diffraction experiment also provide detailed information about the local structure surrounding the nitrogen atom. The coordination number of Fe atom around a nitrogen atom for the iron nitride containing 9.5 at.%N turns out to be 3.9 atoms.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.26 no.3
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• pp.121-125
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• 2016

The effect of temperature and pressure in the nitrogen ambient furnace on bulk micro defect (BMD) and denuded zone (Dz) is experimentally investigated. It is found that as pressure increases, Dz depth increases with a small decrease of BMD density in the range of temperature, $100{\sim}300^{\circ}C$. BMD density with hot isostatic pressure treatment (HIP) at temperature of $850^{\circ}C$ is higher than that without HIP while Dz depth is lower due to much higher BMD density. As the pressure increases, BMD density is increased and saturated to a critical value, and Dz depth increases even if BMD density is saturated. The concentration of nitrogen increases near the surface with increasing pressure, and the peak of the concentration moves closer to the surface. The nitrogen is gathered near the surface, and does not become in-diffusion to the bulk of the wafer. The silicon nitride layer near the surface prevents to inject the additional nitrogen into the bulk of the wafer across the layer. The nitrogen does not affect the formation of BMD. On the other hand, the oxygen is moved into the bulk of the wafer by increasing pressure. Dz depth from the surface is extended into the bulk because the nuclei of BMD move into the bulk of the wafer.