• 한국진공학회:학술대회논문집
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• 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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• pp.181.2-181.2
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• 2014

A single-layer graphene has been uniformly grown on a Cu surface at elevated temperatures by thermally processing a poly (methyl methacrylate) (PMMA) film in a rapid thermal annealing (RTA) system under vacuum. The detailed chemistry of the transition from solid-state carbon to graphene on the catalytic Cu surface was investigated by performing in-situ residual gas analysis while PMMA/Cu-foil samples being heated, in conjunction with interrupted growth studies to reconstruct ex-situ the heating process. We found that the gas species of mass/charge (m/e) ratio of 15 ($CH_3{^+}$) was mainly originated from the thermal decomposition of PMMA, indicating that the formation of graphene occurs with hydrocarbon molecules vaporized from PMMA, such as methane and/or methyl radicals, as precursors rather than by the direct graphitization of solid-state carbon. We also found that the temperature for dominantly vaporizing hydrocarbon molecules from PMMA and the length of time, the gaseous hydrocarbon atmosphere is maintained, are dependent on both the heating temperature profile and the amount of a solid carbon feedstock. From those results, we strongly suggest that the heating rate and the amount of solid carbon are the dominant factors to determine the crystalline quality of the resulting graphene film. Under optimal growth conditions, the PMMA-derived graphene was found to have a carrier (hole) mobility as high as ${\sim}2,700cm^2V^{-1}s^{-1}$ at room temperature, which is superior to common graphene converted from solid carbon.

• 공업화학
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• 제27권1호
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• pp.45-49
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• 2016

과량의 GO 및 poly(4-styrene sulfonate) (PSS)의 존재 하에서 산화제 없이 3,4-ethylenedioxythiophene (EDOT)의 in-situ 중합 반응을 시도하였다. 반응물(GO-P)의 XPS, FT-IR 등의 분석을 통하여 산화제 없이도 모노머인 EDOT의 산화중합이 원활하게 진행되어 PEDOT/PSS가 합성되고 GO와 복합화된 것을 확인할 수 있었다. GO-P는 수분산성은 우수하였으나, 전기적 절연체인 GO가 42% 포함되어 있으므로 전기전도도는 $15S{\cdot}m^{-1}$로 매우 낮았다. 그러나 GO-P 필름을 $200^{\circ}C$에서 8 h 열처리하면 GO의 일부분이 환원되면서 전도도가 $212S{\cdot}m^{-1}$까지 향상되었다.

• 한국재료학회지
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• 제24권3호
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• pp.166-173
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• 2014

The effects of printed circuit board electroless nickel immersion gold (ENIG) and organic solderability preservative (OSP) surface finishes on the electromigration reliability and shear strength of Sn-3.5Ag Pb-free solder bump were systematically investigated. In-situ annealing tests were performed in a scanning electron microscope chamber at 130, 150, and $170^{\circ}C$ in order to investigate the growth kinetics of intermetallic compound (IMC). Electromigration lifetime and failure modes were investigated at $150^{\circ}C$ and $1.5{\times}10^5A/cm^2$, while ball shear tests and failure mode analysis were conducted under the high-speed conditions from 10 mm/s to 3000 mm/s. The activation energy of ENIG and OSP surface finishes during annealing were evaluated as 0.84 eV and 0.94 eV, respectively. The solder bumps with ENIG surface finish showed longer electromigration lifetime than OSP surface finish. Shear strengths between ENIG and OSP were similar, and the shear energies decreased with increasing shear speed. Failure analysis showed that electrical and mechanical reliabilities were very closely related to the interfacial IMC stabilities.

• Journal of Magnetics
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• 제17권4호
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• pp.265-270
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• 2012

We report improved low-field magnetoresistance (LFMR) effects of the $La_{0.7}Sr_{0.3}Mn_{1+d}O_3-Mn_3O_4$ composite films with the nominal composition of $La_{0.7}Sr_{0.3}MnO_3$(LSMO)-50 mol% $Mn_3O_4$. The composite films were fabricated by ex-situ solid phase crystallization (SPC) of amorphous films at the annealing temperature region of $900-1100^{\circ}C$ for 2 h in a pure oxygen atmosphere. The amorphous films were deposited on polycrystalline $BaZrO_3$ (poly-BZO) substrates by dc-magnetron sputtering at room temperature. The Curie temperatures ($T_C$) of all composite films were insignificantly altered in the range of 368-372 K. The highest LFMR value of 1.29 % in 0.5 kOe with the maximum dMR/dH value of $37.4%kOe^{-1}$ at 300 K was obtained from 900 nm-thick composite film annealed at $1100^{\circ}C$. The improved LFMR properties of the composite films are attributed to effective spin-dependent scattering at the $La_{0.7}Sr_{0.3}Mn_{1+d}O_3$ grain boundaries sharpened by adjacent chemically compatible $Mn_3O_4$ grains.

• 한국초전도학회:학술대회논문집
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• 한국초전도학회 2000년도 High Temperature Superconductivity Vol.X
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• pp.201-206
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• 2000

Effects of the post-annealing temperature of CeO$_2$ buffer layers on the properties of YBCO films on CeO$_2$-buffered sapphire were investigated. 45 nm-thick CeO$_2$ buffer layer was prepared in-situ on r-cut sapphire using an on-axis rf magnetron sputtering method, which was later post-annealed at temperatures between 950$^{\circ}$C and 1100$^{\circ}$C in an oxygen-flowing environment. YBCO films were prepared on CeO$_2$-buffered sapphire (CbS), for which the surface morphology, crystal structures and electrical properties of the YBCO films were studied. YBCO films on post-annealed CbS appeared to have better properties than those on as-grown CbS with regard to the morphological, structural and electrical properties when the YBCO films were prepared on CeO$_2$ buffer layer post-annealed at temperatures of 1000 - 1050$^{\circ}$C. A TE$_{011}$ mode rutileloaded cylindrical cavity resonators was fabricated with the YBCO films placed as the endplates, for which the unloaded Q of the resonator was measured. It turned out that the resonator with the endplates prepared from the YBCO films on postannealed CbS at 1000 $^{\circ}$C showed the highest unloaded Q with the value more than 8 ${\times}$ 10$^5$ at 30 K and 8.6 CHz, revealing that the YBCO films on post-annealed CbS at 1000$^{\circ}$C the temperature could be the lowest among the YBCO films on post-annealed CbS.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2000년도 제18회 학술발표회 논문개요집
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• pp.125-125
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• 2000

백금 스퍼터 증착시 아르곤에 산소와 같은 첨가 가스를 사용할 경우 산화막에 대한 접착력이 좋아지며 백금 박막의 우선배향성을 조절할 수 있음이 알려져 있다. 이러한 첨가 가스는 백금 박막에 상당량 포함되며 스퍼터링 후 열처리 과정에서 탈착되는 것으로 알려져 있다. 후열처리 도중 첨가 가스의 탈착 거동이 백금 박막의 미세구조, 조성 및 전기 전도도 등과 같은 제반 물성에 영향을 미칠 것이라 추정된다. 본 연구에서는 백금의 스퍼터링 시 질소를 첨가하여 질소가 포함된 백금 박막을 증착한 후 질소 탈착 거동을 연구하기 위해 실시간 타원해석기(in situ ellipsometer)를 이용하여 진공열처리(15mTorr)하면서 온도변화에 따른 유효굴절율(n)과 소광계수(k) 값을 구하였다. 또한 산소를 첨가하여 얻은 백금 박막의 결과와 비교하여 백금 박막내에 포함된 산소와 질소의 탈착 거동의 차이를 조사하였다. 산소를 이용하여 우선배향성이 (200)으로 조절된 박막의 경우 n과 k의 급격한 변화가 관찰되었으며 이로부터 55$0^{\circ}C$ 온도에서 산소가 급격히 빠져나감을 추측할 수 있었으며 열처리 후에는 백금 bulk 값에 가까운 값을 가짐을 알 수 있었다. 한편, 질소를 사용하여 (200)으로 우선배향성이 조절된 박막의 경우 n,k 값의 후열처리 도중의 변화 양상은 스퍼터링 압력에 크게 의존하는 것으로 나타났다. 22mTorr에서 스퍼터링한 박막의 경우 23$0^{\circ}C$ 부근에서 굴절률과 미세구조의 변화가 있음을 관찰할 수 있었으나, 10mTorr에서 스퍼터링한 시편의 경우 굴절률의 변화양상은 산소를 상요한 경우와 매우 유사한 거동을 나타내지만 열처리 후에는 상대적으로 낮은 n,k 값을 나타내고 있었다. 또한 열처리 시편의 미세구조 변화에 대한 분석 결과 산소 사용의 경우는 측정온도 범위내에서는 후 열처리 후에도 박막내에 hole이나 hillock 등이 관찰되지 않아 bulk 값에 가까운 n, k 값을 가지지만, 질소 사용의 경우는 hole, 표면 거칠기, 혹은 스퍼터링 중에 인입된 질소의 탈착이 완전히 이루어지지 못해 bulk 값과 다르게 나온 것으로 생각된다.

• Transactions on Electrical and Electronic Materials
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• 제18권5호
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• pp.253-256
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• 2017

A thin Te interlayer was applied to a Ni/n-InGaAs contact to reduce the contact resistance between Ni-InGaAs and n-InGaAs. A 5-nm-thick Te layer was first deposited on a Si-doped n-type $In_{0.53}Ga_{0.47}As$ layer, followed by in situ deposition of a 30-nm-thick Ni film. After the formation of the Ni-InGaAs alloy by rapid thermal annealing at $300^{\circ}C$ for 30 s, the extracted specific contact resistivity (${\rho}_c$) reduced by more than one order of magnitude from $2.86{\times}10^{-4}{\Omega}{\cdot}cm^2$ to $8.98{\times}10^{-6}{\Omega}{\cdot}cm^2$ than that of the reference sample. A thinner Ni-InGaAs alloy layer with a better morphology was obtained by the introduction of the Te layer. The improved interface morphology and the graded Ni-InGaAs layer formed at the interface were believed to be responsible for ${\rho}_c$ reduction.

• 한국전기전자재료학회논문지
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• 제20권3호
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• pp.202-206
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• 2007

ZnO is a promising material to make high efficient ultraviolet(UV) or blue light emitting diodes(LEDs) because of its large binding energy and energy bandgap. In this study, we prepared ZnO thin films with p-type conductivity on silicon(100) substrates by RF magnetron sputtering in the mixture of $N_2$ and $O_2$. The process was accompanied by low pressure in-situ annealing in $O_2$ at $600^{\circ}C$ and $800^{\circ}C$ respectively. Hall effect in Van der Pauw configuration showed that the N-doped ZnO film annealed at $800^{\circ}C$ has p-type conductivity. Photoluminescence(PL) spectrum of the film annealed at $800^{\circ}C$ showed UV emission related to exciton and bound to donor-acceptor pair(DAP) as well as visible emission related to many intrinsic defects.

• 한국초전도ㆍ저온공학회논문지
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• 제16권2호
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• pp.24-28
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• 2014

Magnesium diboride superconductor is still of considerable interest because of its appealing characteristics towards application mainly at around 20 K. Unlike Nb-based superconductors, $MgB_2$ can be operated by cryogen-free cooler which provides a cost effective alternative at low field of around 2-5 T. To explore this operating field region considerable efforts are necessary to marginally improve the superconducting properties of $MgB_2$. Under this situation, even the heat treatment environment during the synthesis is considered as an important factor. The addition of $H_2$ gas in small amount with Ar as a mixed gas during annealing has an adverse effect on the superconducting properties of $MgB_2$. It is although interesting to find that the presence of Mg vapor along with hydrogen during heat treatment results in the appreciable improvement in the flux pinning and the overall response of the critical current density for the ex-situ $MgB_2$ samples.

• 마이크로전자및패키징학회지
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• 제29권2호
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• pp.81-89
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• 2022

비전도성 필름(non-conductive film, NCF)의 적용이 Cu/Ni/Sn-2.5Ag 미세범프의 금속간화합물(intermetallic compound, IMC) 성장 거동에 미치는 영향을 분석하기 위해 110, 130, 150℃의 온도 조건과 1.3×10⁵ A/cm²의 전류밀도 조건에서 실시간 열처리 및 electromigration(EM) 실험을 진행하였다. 그 결과, NCF 적용 유무와 열처리 및 EM 실험과 관계없이 Ni₃Sn₄ IMC 성장에 필요한 활성화에너지는 약 0.52 eV로 큰 차이는 보이지 않았다. 이는 Ni-Sn IMC의 성장속도가 Cu-Sn IMC 성장 속도보다 매우 느리며, 또한 Ni-Sn IMC의 성장 거동은 시간의 제곱근에 선형적으로 증가하므로 확산이 지배하는 동일한 반응기구를 가지며 NCF 적용에 따른 역응력(back stress)의 EM 억제 효과가 크지 않기 때문에 Ni₃Sn₄ IMC 성장에 필요한 활성화에너지는 차이가 나지 않는 것으로 판단된다.