• 센서학회지
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• 제1권2호
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• pp.117-123
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• 1992

적층구조의 Pt-Sn 박막을 히터 위에서 열산화하여 $Pt-SnO_{2-x}$ 박막형 CO 가스감지소자를 제조하였다. 열증착법으로 증착된 Sn의 두께는 $4000{\AA}$이었으며 그 위에 D.C. sputtering법으로 증착된 Pt의 두께는 $14{\AA}{\sim}71{\AA}$ 이었다. XRD 분석에서 $Pt-SnO_{2-x}$ 박막은 $200{\AA}$ 정도의 입경과 주방향성이 (110)인 $(SnO_{2}){\cdot}6T$ 결정상을 보였다. $Pt-SnO_{2-x}$ 박막소자(Pt 두께 : $43{\AA}$)는 6000 ppm의 CO에 대해 80% 정도의 감도와 CO에 대해 높은 선택도를 나타내었다. 그리고 CO에 고감도를 갖는 $Pt-SnO_{2-x}$ 박막소자의 열산화 온도와 동작온도가 각각 $500^{\circ}C$와 $200^{\circ}C$이었다.

• 한국세라믹학회지
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• 제37권12호
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• pp.1135-1139
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• 2000

본 연구에서는 Pt/Sn $O_2$박막의 CO 감지특성을 향상시키기 위하여 표면 형상을 제어하였다. Pt/Sn $O_2$계 박막센서의 최적 동작온도는 175$^{\circ}C$이었다. Pt가 12초 동안 증착된 Sn $O_2$가 200ppm의 CO 가스에 대하여 1.23의 최대감도를 나타내었고, 그 이상의 Pt 증착시간 증가에 따라 Sn $O_2$위의 Pt의 coverage가 증가하여 센서의 감도를 감소시켰다. 다층박막(multi-layer thin film)의 단층의 Pt/Sn $O_2$복합체 위에 다시 Sn $O_2$및 Pt의 cluster 층들을 연속적으로 증착함으로서 제작되었다. 단지 하나의 Pt 층만을 증착한 Sn $O_2$막보다 다층의 Pt/Sn $O_2$막이 더욱 우수한 감도( $R_{air}$/ $R_{co}$=1.72, CO: 200 ppm)를 나타내었다. Pt/Sn $O_2$다층박막의 우수한 감도의 원인은 Pt와 Sn $O_2$사이의 계면적 증대 때문인 것으로 생각되어 진다.다.

• Journal of Magnetics
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• 제6권1호
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• pp.19-22
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• 2001

Change of magnetic properties in CoCrPt/Ti perpendicular media with varying CoCrPt film thickness has been studied. As the CoCrPt film thickness increases from 25 nm, the Ms (saturation magnetization) increases rapidly at first and then more gradually. This Ms behavior is associated primarily with the formation of an "amorphous-like"reacted layer created by intermixing of CoCrPt and Ti at the CoCrPt/Ti interface and secondarily with a change of the Cr segregation mode with varying CoCrPt film thickness. Magnetic domain structure distinctively changes with increasing CsCrPt magnetic layer (ML) thickness. Also the strength of exchange coupling measured from the slope in the demagnetizing region of the M-H loop changes with ML thickness. The expansion of lattice parameters a and c at smaller film thickness suggests that the Cr segregation mode may be connected with the residual stress of the films. Finally, the negative nucleation field (Hn) shows a unique behavior with the change of strength of the exchange interaction.teraction.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2016년도 제50회 동계 정기학술대회 초록집
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• pp.143.2-143.2
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• 2016

The influence of electric field on CO adsorbed on Pt(111) was investigated with reflection-absorption infrared spectroscopy (RAIRS) in ultrahigh vacuum system. The ice film capacitor method was used to apply electric field to the amorphous ice film with CO on Pt(111). Two systems were compared by measuring the change of the CO stretching vibrational mode under applied electric field; one is CO on Pt(111), and the other is CO buried inside an ice film on Pt(111). By comparing them, we were able to calculate the additional effect of adsorption of CO on Pt(111) on peak shift. The CO adsorbed on Pt(111) has shown larger peak shift than CO adsorbed with H2O when we applied stronger electric field. Additionally, the differences were observable when the applied electric field exceeds $1{\times}10V/m^8$.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2000년도 International Symposium on Magnetics The 2000 Fall Conference
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• pp.352-362
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• 2000

In this study, effects of novel VMn underlayer on magnetic properties of CoCrPt/VMn longitudinal medium was studied and compared with those of CoCrPt/Cr medium. It was found that the VMn film had (200) preferred orientation and the lattice constant was about 0.2967 nm, which is slightly larger than that of the Cr, 0.2888 nm. The grain size of VMn film was 9.3 nm at 30 nm thickness, and this is about 38 % smaller than that of a similarly deposited Cr film. The CoCrPt/VMn films showed higher coercivity in comparison with the CoCrPt/Cr films. The coercivity increase seems to be attributed to the increased Co (11.0) texture, improved lattice matching between Co (11.0) and VMn (200), and lower stacking fault density. Mn must have diffused into the CoCrPt magnetic layer more uniformly rather than preferentially along grain boundaries this reduced Ms at higher substrate temperature

• 한국표면공학회지
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• 제51권4호
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• pp.243-248
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• 2018

All solid state thin film batteries with two types of cell structure, Pt / $LiCoO_2$ / LiPON / Cu and Pt / $LiCoO_2$ / LiPON / $LiCoO_2$ / Cu, are prepared and their electrochemical performances are investigated to evaluate the effect of $LiCoO_2$ interlayer at the interface of LiPON / Cu. The crystallinity of the deposited $LiCoO_2$ thin films is confirmed by XRD and Raman analysis. The crystalline $LiCoO_2$ cathode thin film is obtained and $LiCoO_2$ as the interlayer appears to be amorphous. The surface morphology of Cu current collector after cycling of the batteries is observed by AFM. The presence of a 10 nm-thick layer of $LiCoO_2$ at the interface of LiPON / Cu enhances the interfacial adhesion and reduces the interfacial resistance. As a result, Li plating / stripping at the interface of LiPON / Cu during charge/discharge reaction takes place more uniformly on Cu current collector, while without the interlayer of $LiCoO_2$ at the interface of LiPON / Cu, the Li plating / stripping is localized on current collector. The thin film batteries with the interlayer of $LiCoO_2$ at the interface of LiPON / Cu exhibits enhanced initial coulombic efficiency, reversible capacity and cycling stability. The thickness of the anode current collector Cu also appears to be crucial for electrochemical performances of all solid state thin film batteries.

• 한국자기학회지
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• 제12권3호
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• pp.94-98
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• 2002

20nm이하의 얇은 박막에서도 높은 보자력이 요구되는 Ti/CoCrPt 수직자기기록박막의 보자력 향상을 위해 Al, Cu, Ni, Cr, Ag, Mg, Fe, Co, Pd, Au, Pt, Mo, Hf등의 여러 하지층과 제조조건이 보자력에 미치는 영향을 조사하였다 이들 중 Ag과 Mg하지층은 Ti/CoCrPt박막의 보자력을 향상시켰으며 특히 2nm Ag 하지층을 사용할 경우 10nm CoCrPt 박막에서 2200 Oe의 높은 보자력을 보일뿐 아니라 $\alpha$값을 낮추는 효과가 있었다. 그러나 Ag를 하지층으로 사용하면 기대와는 달리 Ti(002)면의 우선배향 성장이 전혀 일어나지 않아 보자력 증대에 다른 기구가 작용하는 것으로 판단되었다. 그리고 표면의 거칠기가 큰 기판에서는 보자력뿐만 아니라 역자구생성자계도 감소하였다.

• Journal of Magnetics
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• 제5권4호
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• pp.143-146
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• 2000

In this study, the magnetic properties of CoCrPt films (far longditudinal recording) on a novel VMn underlayer were measured and compared with similar films on conventional Cr underlayers. It was found that the VMn film had (200) preferred orientation and the lattice constant was about 0.2967 nm, which is slightly larger than that of the Cr film, 0.2888 m. The grain size of the VMn film was 9.8 nm at 30 m thickness, about 39% smaller than that of a similarly deposited Cr. The CoCrPt/VMn films showed higher coercivity in comparison with the CoCrPt/Cr films. The coercivity increase is attributed to the increased Co (11.0) texture, improved lattice matching between Co (11.0) and VMn (200), and lower stacking fault density. V or Mn must have diffused into the CoCrPt magnetic layer uniformly rather than preferentially along grain boundaries. This reduced Ms at higher substrate temperature.

• 한국진공학회지
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• 제7권3호
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• pp.176-186
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• 1998

Si 기판 위에 3종의 Pt-Co 합금박막 (Pt66-Co34, Pt40-Co60, Pt18-Co82)과 순수한 Pt, Co 박막 시료를 제작하여 표면 조성분석의 정량화 및 표준화를 위한 표준시료로 제안하 였다. in-istu X-ray photoelectron spectroscopy(XPS)분석에 의해 증착된 이원 합금박막의 조성이 정확히 조절되었으며, 합금박막의 실제 조성은 유도결합플라즈마-원자방출분광법 (inductively coupled plasma-atomic emission spectroscopy: ICP-AES)과 러더퍼드 후방산 란분광법(Ruthford back-scattering spectrometry: RBS)에 의해 결정되었다. in-situ XPS 결과와 ICP에 의한 조성을 비교한 결과 매질 효과를 고려하면 비교적 정확한 조성을 구할 수 있음이 확인되었다. 이 시료를 이용한 XPS와 Auger electron spectroscopy(AES)에 의한 국내 공동분석 결과는 약4%내외의 큰 편차를 보이고 있지만, 평균 조성 값은 약1%의 오차 범위 내에서 두 방법에 의한 결과가 서로 잘 일치하였다. 이온빔 스퍼터링에 의해 Pt조성이 증가된 표면층이 형성되어 정확한 조성분석을 위해서는 선택스퍼터링에 의한 표면 변형을 정량적으로 함을 알았다.

• Journal of Magnetics
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• 제15권1호
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• pp.12-16
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• 2010

Combined study of in-situ stress measurements and atomic force microscopy (AFM) revealed drastic stress relaxation in the CoCrPt and PS(styrene)-PVP(vinyl pyridine) polymer hybrid structure that was closely related to the growth structure of the film. We have observed not only no large initial growth stress at the initial stages of film growth but also twice smaller stress in magnitude with opposite sign in the CoCrPt/PS-PVP/Si sample. The microstructural studies using AFM at the various film growth stages revealed that the film growth structure plays an important role in the stress relaxation mechanism of CoCrPt films on a corrugated polymer surface.