• 한국재료학회지
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• 제10권4호
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• pp.270-275
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• 2000

Metal/ferroelectric/insulator/semiconductor(MFIS)-Field Effect Transistor을 위한 Pt/YMnO$_3$/Y$_2$O$_3$/Si 구조를 제조하여 MFIS 구조의 특성에 미치는 $Y_2$O$_3$박막의 영향을 고찰하였다. PLD법을 이용하여 p=type Si(111) 기판 위에 증착시킨 $Y_2$O$_3$박막은 증착온도와 관계없이 (111)방향으로의 우선배향성을 갖고 결정화 되었다. 실리콘 위에 바로 MOCVD법에 의해 강유전체 YMnO$_3$박막을 증착시킨 경우 실리콘과의 계면에서 Mn이 부족한 층이 형성되지만 $Y_2$O$_3$가 실리콘과 YMnO$_3$사이에 삽입된 경우는 $Y_2$O$_3$바로 위에서부터 화학양론비에 일치하는 양질의 YMnO$_3$박막을 얻을 수 있었다. 85$0^{\circ}C$, 100mtorr의 진공분위기에서 열처리한 YMnO$_3$박막은 $Y_2$O$_3$가 삽입된 경우 memory window 값이 $Y_2$O$_3$가 삽입되지 않은 경우보다 더 큰 값을 보였으며 5V에서 1.3V의 값을 보였다.

• Progress in Superconductivity
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• 제11권2호
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• pp.100-105
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• 2010

Reel-to-reel deposition of $Y_2O_3$ has been performed on Ni-5%W metal substrates using the RF-sputtering method. The epitaxial orientation of $Y_2O_3$ buffer layers to the base bi-axially textured substrate was well identified using ${\theta}-2{\theta}$, out-of-plane ($\omega$), and in-plane ($\phi$) scans in X-ray diffraction analysis. The optimization of $Y_2O_3$ seed layers in reel-to-reel fashion were investigated varying the deposition temperature, sputtering power, and pressure for its significant roles for the following buffer stacks and superconducting layers. $Y_2O_3$ were all grown epitaxially on bi-axially textured metal substrates at 380 watts and 5 mTorr in the temperature range of $600-740^{\circ}C$ with higher $Y_2O_3$ (400) intensities at ${\sim}710^{\circ}C$. It was found that the $\Delta\omega$ values were $1-2^{\circ}$ lower but the $\Delta\phi$ values were above $1^{\circ}$ higher than that of Ni-W substrates. As the sputtering power increased from 340 to 380 watts, $\Delta\omega$ and $\Delta\phi$ values showed decreased tendency. Even in the small window of deposition pressure of 3-7 mTorr, the $Y_2O_3$ (400) intensities increased and $\Delta\omega$ and $\Delta\phi$ values were reduced as sputtering pressure increased.

• 한국세라믹학회지
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• 제42권3호
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• pp.178-181
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• 2005

Silicon oxynitride (SiON) 막은 플라즈마 화학기상증착법(PECVD)으로 $SiH_4,\;N_2O$와 $N_2$ 가스를 사용하여 $SiO_2/Si$ 위해 증착되었다. 증착 변수에 따라서 SiON 막의 굴절률은 prism coupler를 사용하여 1552nm 파장에서 $1.4480\~1.4958$까지 변화하였다. 평판 광도파로 코어로 사용되는 SiON 막의 두께는 $6{\mu}m$이고, buffer 막과의 굴절률 차이(An)는 $0.36\%$이다. 또한 식각 공정으로 $SiO_2$ 막 위에 증착된 SiON 막은 건식식각을 통해서 수행되었다. 광화이버에 $1.55{\mu}m$ 파장의 레이저론 입력단에 조사하였다. 결과적으로 저굴절률 차이 SiON 광도파로를 제작하였으며, 출력단에서 single-mode 형상을 확인하였다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2008년도 하계학술대회 논문집 Vol.9
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• pp.419-420
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• 2008

In this study, high quality (Al,N)-codoped p-type ZnO thin films were obtained by DC magnetron sputtering. The film on buffer layer grown in 80% $N_2$ ambient shows highest hole concentration of $2.93\times10^{17}cm^{-3}$. The films show hole concentration in the range of $1.5\times10^{15}$ to $2.93\times10^{17}cm^{-3}$, resistivity of 131.2 to 2.864 $\Omega$cm, mobility of 3.99 to 31.6 $cm^2V^{-1}s^{-1}$. The films on Si show easier p-doping in ZnO than those on buffer layer. The film on Si shows the highest quality of optical photoluminescence (PL) characteristics. The donor energy level $(E_d)$ of (Al,N)-codoped ZnO films is about 50 meV and acceptor energy level $(E_a)$ is in the range of 63 to 71 meV. It will help to improve p-type ZnO films.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 하계학술대회 논문집
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• pp.263-266
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• 2001

In this paper, we investigated dielectric properies for BST thin films that was deposited on MgO/Si substrates using RF magnetron sputtering. In here, MgO film was used to perform that a diffusion b arrier between the BST film and Si substrate and a buffer layer to assist the BST film growth. A d eposition condition for MgO films was RF Power of 50W, substrate temperature of room temperature and the working gas ratio of Ar:O$_2$ were varied from 90:10 to 60:47. Finally we manufactured the cap acitor of Al/BST/MgO/Si/Al structure to know electrical properties of this capacitor through I-V, C-V measurement. In the results, C-V aha racteristic curves was shown a ferroelectric property so we measured P-E. A remanent poliazation and coerceive electric field was present 2$\mu$C/cm$^2$ and -27kV/cm respectively at Ar:O$_2$=90:10. And a va clue of dielectric constant was 86 at Ar:02=90:10.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2008년도 추계학술대회 논문집 Vol.21
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• pp.273-273
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• 2008

This paper describes the frequency response of two-port surface acoustic wave (SAW) resonator made of 002-polycrystalline aluminum nitride (AlN) thin film on 111-poly 3C-SiC buffer layer. In there, Polycrystalline AlN thin films were deposited on polycrystalline 3C-SiC buffer layer by pulsed reactive magnetron sputtering system, the polycrystalline 3C-SiC was grown on $SiO_2$/Si sample by CVD. The obtained results such as the temperature coefficient of frequency (TCF) of the device is about from 15.9 to 18.5 ppm/$^{\circ}C$, the change in resonance frequency is approximately linear (30-$150^{\circ}C$), which resonance frequency of AlN/3C-SiC structure has high temperature stability. The characteristics of AlN thin films grown on 3C-SiC buffer layer are also evaluated by using the XRD, and AFM images.

• 센서학회지
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• 제16권6호
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• pp.457-461
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• 2007

This paper describes the characteristics of poly (polycrystalline) 3C-SiC grown on $SiO_{2}$ and AlN substrates, respectively. The crystallinity and the bonding structure of poly 3C-SiC grown on each substrate were investigated according to various growth temperatures. The crystalline quality of poly 3C-SiC was improved from resulting in decrease of FWHM (full width half maximum) of XRD and FT-IR by increasing the growth temperature. The minimum growth temperature of poly 3C-SiC was $1100^{\circ}C$. The surface chemical composition and the electron mobility of poly 3C-SiC grown on each substrate were investigated by XPS and Hall Effect, respectively. The chemical compositions of surface of poly 3C-SiC films grown on $SiO_{2}$ and AlN were not different. However, their electron mobilities were $7.65{\;}cm^{2}/V.s$ and $14.8{\;}cm^{2}/V.s$, respectively. Therefore, since the electron mobility of poly 3C-SiC films grown on AlN buffer layer was two times higher than that of 3C-SiC/$SiO_{2}$, a AlN film is a suitable material, as buffer layer, for the growth of poly 3C-SiC thin films with excellent properties for M/NEMS applications.

• 마이크로전자및패키징학회지
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• 제21권1호
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• pp.7-11
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• 2014

최근 유기태양전지의 효율향상을 위하여 고분자의 PEDOT:PSS 양극(Anode) 버퍼층이 널리 사용되고 있다. 그러나 고효율 태양전지의 개발과 더불어 새로이 적용되고 있는 역구조 유기 태양전지에는 이 같은 친수성의 PEDOT:PSS 고분자가 소수성의 양극이나 광활성층 상에 균일하게 코팅되는 것이 문제점으로 지적되고 있다. 이러한 문제점을 극복하기 위해서 양극 버퍼층으로 $V_2O_5$와 같은 p-type 금속산화물을 사용한 연구가 많이 보고되고 있다. 본 연구에서는 저항을 낮추고 홀 이동도를 향상 시키기 위해 Ag를 삽입층으로 한 $V_2O_5$/Ag/ITO 구조의 다층 박막을 제작하고 Ag두께에 따른 전기적, 광학적, 구조적 특성의 변화에 대하여 살펴보았다. 가시광 영역에서는 Ag 두께가 증가함에 따라 광 투과율이 감소하는 반면 전기적 특성은 향상되는 것을 볼 수 있었다. 광소자의 투명전극산화물로 적합한 구조인지 평가하기 위해 Figure Of Merit(FOM)의 값을 측정하였고, 그 결과 Ag의 두께가 4 nm에서 가장 좋은 특성을 나타냈다. $V_2O_5$/Ag/ITO 구조의 다층 박막은 가시광 영역에서 Ag의 두께가 4 nm일 때 88%의 광 투과율을 나타내었고 저항 값은 $4{\times}10^{-4}{\Omega}cm$로써 광소자로 적합한 구조임을 확인하였다.

• 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.

• 한국초전도학회:학술대회논문집
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• 한국초전도학회 2006년도 High Temperature Superconductivity Vol.XVI
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• pp.71-71
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• 2006