• 한국세라믹학회지
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• 제42권4호
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• pp.219-223
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• 2005

A promising capacitor, which has conformable step coverage and good uniformity of thickness and composition, is needed to manufacture high-density non-volatile FeRAM capacitors with a stacked cell structure. In this study, ferroelectric $Bi_{3.61}Nd_{0.39}Ti_3O_{12}$ (BNdT) thin films were prepared on $Pt(111)/TiO_2/SiO_2/Si$ substrates by the liquid delivery system MOCVD method. In these experiments, $Bi(ph)_{3}$, $Nd(TMHD)\_{3}$ and $Ti(O^iPr)_{2}(TMHD)_{2}$ were used as the precursors and were dissolved in n-butyl acetate. The BNdT thin films were deposited at a substrate temperature and reactor pressure of approximately $600^{\circ}C$ and 4.8 Torr, respectively. The microstructure of the layered perovskite phase was observed by XRD and SEM. The remanent polarization value (2Pr) of the BNdT thin film was $31.67\;{\mu}C/cm^{2}$ at an applied voltage of 5 V.

• 한국진공학회지
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• 제11권4호
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• pp.201-206
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• 2002

N형 InGaAs에 대한 Pd/Si/Pd/Ti/Au 오믹 접촉의 급속 열처리 조건에 따른 오믹 특성을 조사하였다. $450^{\circ}C$까지의 열처리 동안에 전반적으로 우수한 오믹 특성을 나타내어 $400^{\circ}C$, 20초의 급속 열처리 조건에서 최저 $3.9\times10^{-7}\Omega\textrm{cm}^2$ 의 접촉 비저항을 나타내었다. 이는 열처리에 의해 생성된 Pd-Si계 화합물의 형성 및 Si의 InGaAs 표면으로의 확산과 관련이 있었다. 그러나 $400^{\circ}C$에서 열처리 시간을 30초 이상으로 연장할 경우 접촉 비저항이 low-$10^{-6}\Omega \textrm{cm}^2$ 으로 약간 증가하였고, 열처리 조건을 425~$450^{\circ}C$/10초로 변화시킬 경우 high-$10^{-7}$~low-$10^{-6}\Omega \textrm{cm}^2$으로 약간 증가하였다. 이는 오믹 재료와 InGaAs의 반응에 의해 Pd-Ga계 화합물이 형성된 것과 관련이 있었다. 고온 열처리 후에도 오믹 재료와 InGaAs의 평활한 계면을 유지하면서 우수한 오믹 특성을 나타내어, 화합물 반도체 소자의 오믹 접촉으로 충분히 응용 가능하다고 판단된다.

• 한국반도체및디스플레이장비학회:학술대회논문집
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• 한국반도체및디스플레이장비학회 2006년도 추계학술대회 발표 논문집
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• pp.166-169
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• 2006

A promising capacitor, which has conformable step coverage and good uniformity of thickness and composition, is needed to manufacture high-density non-volatile FeRAM capacitors with a stacked cell structure. In this study, ferroelectric $Bi_{3.61}Nd_{0.39}Ti_3O_{12}$ (BNT) thin films were prepared on $Pt(111)/Ti/SiO_2/Si$ substrates by the liquid delivery system MOCVD method. In these experiments, $Bi(ph)_3$, $Nd(TMHD)_3$ and $Ti(O^iPr)_2(TMHD)_2$ were used as the precursors and were dissolved in n-butyl acetate. The BNT thin films were deposited at a substrate temperature and reactor pressure of approximately $600^{\circ}C$ and 4.8 Torr, respectively. The microstructure of the layered perovskite phase was observed by XRD and SEM. The remanent polarization value (2Pr) of the BNT thin film was $31.67\;{\mu}C/cm^2$ at an applied voltage of 5 V.

• 대한전자공학회:학술대회논문집
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• 대한전자공학회 2004년도 하계종합학술대회 논문집(2)
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• pp.371-374
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• 2004

In this paper, Ni Germane-silicide formed on undoped $Si_{0.8}Ge_{0.2}$ as well as source/drain dopants doped $Si_{0.8}Ge_{0.2}$ was characterized by the four-point probe for sheet resistance. x-ray diffraction (XRD), x-ray photoelectron spectroscopy (XPS) and field emission scanning electron microscope (FESEM). Low resistive NiSiGe is formed by one step RTP (Rapid thermal processing) with temperature range at $500{\~}700^{\circ}C$. To enhance the thermal stability of Ni Germane-silicide, Ni/Co/TiN structure with different Co concentration were studied in this work. Low sheet resistance was obtained by Ni/Co/TiN structure with high Co concentration using 2-step RTP and it almost keeps the same low sheet resistance even after furnace annealing at $650^{\circ}C$ for 30 min.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2005년도 하계학술대회 논문집 Vol.6
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• pp.205-206
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• 2005

PRAM (Phase change Random Access Memory) is one of the most promising candidates for next generation Non-volatile Memories. The Phase change material has been researched in the field of optical data storage media. Among the phase change materials, $Ge_2Sb_2Te_5$(GST) is very well known for its high optical contrast in the state of amorphous and crystalline. However, the characteristics required in solid state memory are quite different from optical ones. In this study, the structural properties of GST thin films with bottom electrode were investigated for PRAM. The 100-nm thick GST films were deposited on TiN/Si and TiAlN/Si substrates by RF sputtering system. In order to characterize the crystal structure and morphology of these films, we performed x-ray diffraction (XRD) and atomic force microscopy (AFM).

• 한국진공학회지
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• 제10권3호
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• pp.368-373
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• 2001

N형 InGaAs에 대한 Pd/Si/Ti/Pt 오믹 접촉 특성을 조사하였다. 증착 상태에서는 접촉 비저항을 측정할 수 없을 정도의 비오믹 특성을 보였으며, $375^{\circ}C$에서 10초 동안 열처리한 경우 $5\times10^{-3}\Omega\textrm{cm}^2$의 높은 접촉 비저항을 나타내었다. 그러나 열처리 시간을 60초로 연장할 경우 접촉 비저항이 $1.7\times10^{-6}\Omega\textrm{cm}^2$로 급격히 감소하였고, 열처리 조건을 $425^{\circ}C$, 10초로 변화시킬 경우 $2\times10^{-6}\Omega\textrm{cm}^2$의 접촉 비저항을 나타내었다. 또한 $450^{\circ}C$까지도 오믹 재료와 InGaAs의 평활한 계면을 유지하면서 우수한 오믹 특성을 나타내어, 화합물 반도체 소자의 오믹 접촉으로 충분히 응용가능하다.

• Bulletin of the Korean Chemical Society
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• 제25권11호
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• pp.1661-1666
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• 2004

The reaction of titanium tetraisopropoxide with 2 equiv of N,N-diethyl acetoacetamide affords Ti($O^iPr)_2(CH_3COCHCONEt_2)_2$ (1) as colorless crystals in 80% yield. Compound 1 is characterized by spectroscopic (Mass and $^1H/^{13}C$ NMR) and microanalytical data. Molecular structure of 1 has been determined by a single crystal X-ray diffraction study, which reveals that it is a monomeric, cis-diisopropoxide and contains a six coordinate Ti(IV) atom with a cis($CONEt_2$), trans($COCH_3$) configuration (1a) in a distorted octahedral environment. Variable-temperature $^1H$ NMR spectra of 1 indicate that it exists as an equilibrium mixture of cis, trans (1a) and cis, cis (1b) isomers in a 0.57 : 0.43 ratio at -20$^{\circ}C$ in toluene-$d_8$ solution. Thermal properties of 1 as a MOCVD precursor for titanium dioxide films have been evaluated by thermal gravimetric analysis and vapor pressure measurement. Thin films of pure anatase titanium dioxide (after annealing above 500$^{\circ}C$ under oxygen) have been grown on Si(100) with precursor 1 in the substrate temperature range of 350- 500$^{\circ}$ using a bubbler-based MOCVD method.

• 한국전기전자재료학회논문지
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• 제37권1호
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• pp.88-93
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• 2024

To evaluate the possibility as a multi-level memory medium for the Ge₂Sb₂Te₅/TiN/W-doped Ge₂Sb₂Te₅ cell structure, the crystallization rate and stabilization characteristics according to voltage (V)- and current (I)- pulse sweeping were investigated. In the cell structures prepared by a magnetron sputtering system on a p-type Si (100) substrate, the Ge₂Sb₂Te₅ and W-doped Ge₂Sb₂Te₅ thin films were separated by a barrier metal, TiN, and the individual thicknesses were varied, but the total thickness was fixed at 200 nm. All cell structures exhibited relatively stable multi-level states of high-middle-low resistance (HR-MR-LR), which guarantee the reliability of the multilevel phase-change random access memory (PRAM). The amorphousto-multilevel crystallization rate was evaluated from a graph of resistance (R) vs. pulse duration (T) obtained by the nanoscaled pulse sweeping at a fixed applied voltage (12 V). For all structures, the phase-change rates of HR→MR and MR→LR were estimated to be approximately t<20 ns and t<40 ns, respectively, and the states were relatively stable. We believe that the doublestack structure of an appropriate Ge-Sb-Te film separated by barrier metal (TiN) can be optimized for high-speed and stable multilevel PRAM.

• 한국결정성장학회지
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• 제6권3호
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• pp.318-326
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• 1996

본 연구는 초고집적회로의 금속 배선으로써 보다 유용할 것으로 기대되는 구리박막의 화학적인 증착기술에 관한 것으로 precursor 물질로는 (hfac)Cu(I)VTMS ; (hevaflouoroacetylacetonate trimethyvinylsilane copper)로 명명된 금속 유기 물질을 사용하였다. 실험시스템의 초기 압력은 $10^{-6}$ Torr를 유지하고, 시스템의 챔버압력과 기판온도가 조정 가능하도록 설계, 제작되었다. 공정 조건에 따른 구리 박막 결정의 성장속도, Grain size, 전기적 성질을 측정하였다. 구리 박막을 증착하기 전에 W(tungsten) 또는 TiN(titanium nitride)이 증착되어 있는 실리콘 웨이퍼를 사용하였다. 본 연구에서는 $250^{\circ}C$이하의 상대적으로 낮은 실리콘 웨이퍼 온도에서의 실험이 가능하였으며 헬륨을 carrier gas로 사용하였는데 연구 결과 구리 박막 증착율이 $220^{\circ}C$에서 최대 $1,800\;{\AA}/분$으로 증가한 반면 표면 거칠기는 $200\;{\AA}$를 갖는 다결정 구리 박막을 관찰하게 되었다. 기판 온도가 $250^{\circ}C$이하일 때의 W(또는 TiN)과 $SiO_{2}$ 기판사이에서 구리 증착 선택성이 관찰되었으며, 최적의 기판 증착 온도는 약 $180^{\circ}C$와 반응용기 압력 0.8 Torr로 나타났다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2004년도 하계학술대회 논문집 Vol.5 No.2
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• pp.965-968
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• 2004

Effective transverse Piezoelectric Coefficients $(e_{31,f})$ of thick PZT $(Pb(Zr_{0.52}Ti{0.48}Ti_{0.48})O_3)$ films on $SiN_x/Si$ substrates were measured with PZT thicknesses and top electrode dimensions. $e_{31,f}$ is one of important Parameters characterizing Piezoelectricity of PZT films. Thick PZT films have been used as various sensors and actuators because of their high driving force and high breakdown voltage. Thick PZT films were fabricated on Pt/Ta/$SiN_x$/Si substrates using sol-gel method. Thicknesses of PZT films were $1{\mu}m$ and $1.8{\mu}m$. $|e_{31,f}|$ values of $1.8{\mu}m$-thick-PZT films were higher than those of $1{\mu}$-thick-PZT films. Maximum $|e_{31,f}|$ of $1.8{\mu}$-thick-PZT films was about $50^{\circ}C/m^2$.