• 대한화학회지
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• 제37권6호
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• pp.570-576
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• 1993

물 표면 위의 스테아르산 단분자막을 은을 입힌 유리판에 이전시켜 1층, 3층, 9층 및 21층의 Langmuir-Blodgett(LB) 분자막을 제조하였다. 표면압은 30 mN/m 이었으며 FTIR-RA 분광법을 이용하여 31~72$^{\circ}C$에서 적외선 흡수 스펙트럼을 얻었다. $31^{\circ}C$에서 탄화수소 사슬이 보다 더 수직적인 배향을 나타내고 있었으며 1층의 경우에는 C = O의 피크가 관찰되지 않았다. 이는 은표면에서 이미지 이중극 효과나 금속염을 형성하기 때문으로 본다. 1층과 3층의 경우에는 스테아르산의 트란스 이성질체가 많고 21층의 경우에는 시스형이 많은 것으로 나타났다. 온도 변화에 대한 FTIR-RAS 측정에서 분자층의 수를 증가시키면 사슬의 녹는점이 높아졌으나 1층의 경우는 예외를 나타내는데 이는 1층의 경우 은기판과의 강한 상호작용에 의한 때문이다.

• 한국광물학회지
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• 제17권4호
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• pp.309-325
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• 2004

연구는 호주 퀸즈랜드 주 북서부에 위치하는 은-납-아연 캔닝턴 광상은 호상편마암, 미그마타이트, 규선석-석류석 편암 그리고 각섬암으로 구성된 모암 주변부에서 발달해 있다. 모암에서 산출되는 규선석의 세 가지 다른 결정형태, 규선석을 포획광물로 함유한 아연-첨정석과 석류석 반상변정은 모암의 변성작용과 아연과 관련된 광화작용에 대한 지질학적 지시자로 사용되었다. 변성작용과 아연 광화작용과의 관계는 프로그램 THERMOCALC를 이용하여 KFMASH (K$_2$O-FeO-MgO-A1$_2$O$_3$-SiO$_2$- $H_2O$), KFMASHTO (K$_2$O-FeO-MgO-A1$_2$O$_3$-SiO$_2$-$H_2O$-TiO$_2$-Fe$_2$O$_3$), NCKFMASH ($Na_2$O-CaO-K$_2$O-FeO-MgO-Al$_2$O$_3$-SiO$_2$-$H_2O$) 그리고 MnNCKFMASH (MnO-$Na_2$O-CaO-K$_2$O-FeO-MgO-Al$_2$O$_3$-SiO$_2$-$H_2O$) 화학계에서 이들 세 가지 광물의 공생관계와 규선석-석류석-부분용융의 상평형 관계를 이용하여 결정하였다. MnNCKFMASH와 NCKFMASH계에서 부분 용융은 KFMASH와 KFMASHTO계에서 보다 낮은 온도에서 일어나며, MnNCKFMASH 계에서 용융 온도는 암석 화학 성분의 Na+Ca+K)의 비가 증가함에 따라 감소하는 경향을 보인다. 캔닝턴 광상의 모암은 MnNCKFMASH계의 경우 최고 온도와 압력 환경에서(634$\pm$62$^{\circ}C$, 4.8$\pm$1.3 kbar) 약 15% 용융되지만, KFMASHTO계하에서는 부분 용융이 일어나지 않는다. 규선석의 등변성도선과 모드 비의 변화를 근거로, 주상과 능면형의 규선석과 주상의 규선석을 포획하는 아연-첨정석 반상변정은 부분 용융을 포함하는 온도와 압력의 증가(약 550～$600^{\circ}C$, 2.0～3.0 kbar에서 700～75$0^{\circ}C$, 5.0～7.0 kbar)로 인한 것으로 생각된다. 또한 이와 같은 변성작용 동안의 최대 수축 변형 방향은 남-북 그 다음 동서 방향으로 주로 D$_1$과 D$_2$ 변형작용 동안에 형성되어졌다. 결론적으로 아연-첨정석의 성장과 관련된 아연 광화 작용은 D$_2$ 동안에 일어났고 그 후 부분 용융과 후기 변형/변성작용에 의해 재배치 또는 재농집 되어진 것으로 생각된다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2016년도 제50회 동계 정기학술대회 초록집
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• pp.85.2-85.2
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• 2016

With the advent of ultra-short high-intense XFEL (X-ray Free Electron Laser), time-resolved dynamics has become of great importance in exploring femtosecond real-world phenomena of nanoscience and biology. These include studying the response of materials to femtosecond laser excitation and investigating the interaction of XFEL itself with condensed matter. A variety of dynamic phenomena have been investigated such as radiation damage, ultrafast melting process, non-equilibrium phase transitions caused by orbital-lattice-spin couplings. As far as bulk materials are concerned, the sample size has no effect on the following dynamic process. As a result, imaging information is not required by and large. If the sample size is of tens of nanometers, however, sample starts to experience quantum confinement effect which, in turn, affects the following dynamic process. Therefore, to understand the fundamental dynamic phenomena in nano-science, time-resolved imaging information is essential. In this talk, we will briefly introduce scientific highlights achieved in XFEL-based dynamics. In case of bio-imaging, recent scientific topics will be mentioned as well. Finally, we will aim to present feasible topics in ultrafast time-resolved imaging and to discuss the future plan of CXI beamline at PAL-XFEL.

• 한국재료학회지
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• 제19권2호
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• pp.95-101
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• 2009

Glass ceramics were made from coal bottom ash by adding CaO and $Li_2O$ as glass modifiers and $TiO_2$ as a nucleating agent in a process of melting and quenching followed by a thermal treatment. The surface of the glass ceramics has 1.6 times more $Li_2O$ compared to the inner matrix. When $TiO_2$ was not added or when only 2 wt% was added, the surface parts of the glass ceramics were crystalline with a thickness close to $130{\mu}m$. In addition, the matrixes showed only the glass phase and not the crystalline phase. However, doping of $TiO_2$ from 4 wt% to 10 wt% began to create small crystalline phases in the matrix with an increase in the quantity of the crystalline. The matrix microstructure of glass ceramics containing $TiO_2$ in excess of 8 wt% was a mixture of dark-gray crystalline and white crystalline parts. These two parts had no considerable difference in terms of composition. It was thought that the crystallization mechanism affects the crystal growth, direction and shape and rather than the existence of two types of crystals.

• Macromolecular Research
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• 제17권5호
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• pp.346-351
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• 2009

$TiCl(O-i-Pr)_3/SiO_2$ and $Ti(O-i-Pr)_4/SiO_2$ were prepared by immobilizing chlorotitanium (IV) isopropoxide ($TiCl(O-i-Pr)_3$) and titanium (IV) isopropoxide ($Ti(O-i-Pr)_4$), to pretreated silica. The effect of the polymerization reaction conditions on the catalytic activity and characteristics of the resulting PLA were investigated. The catalytic conversion, molecular weight and polydispersity index (PDI) of the PLA produced on the titanium alkoxide supported catalysts increased proportionally with the reaction temperature. When the PLA was synthesized in bulk polymerization, the PLA produced with the supported catalysts had higher molecular weight than those with homogeneous catalysts. The melting temperature of the polymer produced with silica supported alkoxide catalysts was approximately $170-180^{\circ}C$.

• 한국재료학회지
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• 제15권2호
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• pp.79-84
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• 2005

The lowest activation temperature of a commercial vacuum getter reported so far in literature was about $400^{\circ}C$. Recently, $Ti_{0.3}Zr_{0.2}V_{0.5}$ alloy has been reported to exhibit the activation temperature lower than $200^{\circ}C$ when they are prepared as thin film. In this study, the alloy was prepared as bulk form and its activation temperature and hydrogen sorption properties were investigated in compliance with a standard method. The alloy powder was prepared by arc melting and subsequent HDH(Hydride-DeHydride) process. The activation temperature of the alloy was estimated from the ultimate pressure-temperature curve and located between $150^{\circ}C\;and\;200^{\circ}C$. The hydrogen sorption speed measured by an orifice method was 0.895 liter/sec which is comparable to thin film of same composition.

• 한국세라믹학회지
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• 제21권3호
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• pp.231-238
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• 1984

Heavy metal fluoride glasses exhibit considerable promise as high transparency materials from the UV to the IR. These glasses are prepared by fusion of the mixture of metal fulorides($ZrF_4$, $BaF_2$, $LaF_3$ etc) at 800-1, 00$0^{\circ}C$ under the inert$(N_2)$ or reactive ($CCl_4$, $Cl_2$) atmosphere following the casting into glass on cooling. Infrared absorption at the 3, 400 cm-1 -OH peak has been measured as a function of thickness for several ZrF-$BaF_2$-LaF and $HfF_4$-$BaF_2$-$LaF_3$ glasses to separate contributions from bulk and surface -OH. For glasses melted under $CCl_4$ reactive atmosphere the peak is due almost entirely to surface-OH. and melting in a closed reactor was best for removing -OH. In ambient atmosphere the -OH peak exhibited no time dependence over a 30 d period indicating a very small rate of surface attack by atmospheric H2O. Removal of -OH absorption processing was generally easier and more complete for the $BaF_2$/ThF4-glasses than for the $ZrF_4$-or $HfF_4$-based glasses.

• Journal of Magnetics
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• 제20권4호
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• pp.336-341
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• 2015

MnBi alloys were fabricated by arc melting and annealing at 573 K. The heat treatment enhanced the content of the low-temperature phase (LTP) of MnBi up to 83 wt%. The Bi-excess assisted LTP MnBi alloys were used in the hybridization with the Nd-Fe-B commercial Magnequench ribbons to form the hybrid magnets (100-x)NdFeB/xMnBi, x = 20, 30, 40, 50, and 80 wt%. The as-milled powder mixtures of Nd-Fe-B and MnBi were aligned in a magnetic field of 18 kOe and warm-compacted to anisotropic and dense bulk magnets at 573 K by 2,000 psi for 10 min. The magnetic ordering of two hard phase components strengthened by the exchange coupling enhanced the Curie temperature ($T_c$) of the magnet in comparison to that of the powder mixture sample. The prepared hybrid magnets were highly anisotropic with the ratio $M_r/M_s$ > 0.8. The exchange coupling was high, and the coercivity $_iH_c$ of the magnets was ~11-13 kOe. The maximum value of the energy product $(BH)_{max}$ was 8.4 MGOe for the magnet with x = 30%. The preparation of MnBi alloys and hybrid magnets are discussed in details.

• 자원환경지질
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• 제27권5호
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• pp.459-467
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• 1994

울산지역에 분포하는 가대리 화강암체는 울산 철 텅그스텐 광화작용의 관계화성암으로서 전형적인 미문상조직을 보여주며, 칼크-알칼리 계열과 I-type화강암류의 지화학적 특성을 나타내고 있다. 가대리화강암은 물이 포화된 상태에서 0.5~2.0 kbar의 압력조건하에서 생성된 것으로 이는 천부에서의 분별결정에 기인된 것으로 화학성분의 분화는 대부분 알칼리 장석의 분별결정작용으로 이루어졌다. 경상분지 최남단에 분포하며 철광화작용과 관련된 미문상화강암체인 마산-김해 화강암체와 가대리화강암제는 미량성분의 화학조성을 비교해볼때 전혀다른 모마그마에서 분화되었음올 시사해준다.

• 한국세라믹학회지
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• 제43권8호
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• pp.486-491
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• 2006

A new $TiN-Ti_5Si_3$ bulk composite was synthesized from preceramic, inorganic polymer (methylpolysilsesquioxane) and $TiH_2$ filler powders via polymer pyrolysis. Using this process, ceramics with high melting points can be produced relatively easily to a near net shape. The $TiN-Ti_5Si_3$ composite oxidized slowly during heating to $1000^{\circ}C$. During heating at the temperatures of at 700 and $800^{\circ}C$, TiN oxidized to Rutile-$TiO_2$ whereas $Ti_5Si_3$ resisted to oxidation. The oxide scale formed consisted primarily of $TiO_2$ containing $Ti_5Si_3$.