• Journal of the Korean Ceramic Society
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• v.37 no.11
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• pp.1126-1129
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• 2000

The crystallographic orientations of $Ba_{0.6}$S $r_{0.4}$Ti $O_3$(BST) thin film deposited by a metal-organic chemical vapor deposition on (111) textured Pt electrode were studied with a transmission electron microscopy. The fully crystallized BST thin film (50nm) has (100) and (110) preferred orientations. A high resolution transmission electron microscopy study has revealed the crystallographic orientation relationships between BST thin film and Pt electrode. These relationships explained the preferred orientation of BST film on (111) textured Pt electrode. With these results, we could represent the atomic arrangement at the BST/Pt interface.e.e.

• Proceedings of the Korean Vacuum Society Conference
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• 2012.08a
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• pp.139-139
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• 2012

With angle resolved photoemission spectroscopy (ARPES), the surface electronic band structures of Pt3Co (111) and Pt3Ni (111) single crystals are investigated, which allow to study the bonding interaction between chemically absorbed atomic oxygen and its surfaces. The d-band electrons of subsurface TM are separated from the direct chemical bonding with atomic oxygen. That is, the TM does not contribute to direct chemical bonding with oxygen. From the density functional theory (DFT) calculations, it is identified that the main origin of improved oxygen absorption property, i.e. softening of Pt-O bonding, is due to the suppression of Pt surface-states which is generated from change of interlayer potential, i.e. charge polarization, between Pt-top and TM-subsurface. Our results point out the critical roles of subsurface TM in modifying surface electronic structures, which in turn can be utilized to tune surface chemical properties.

• Proceedings of the Materials Research Society of Korea Conference
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• 1993.05a
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• pp.64-65
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• 1993

MPB 조성영역인 Zr/Ti=52/48의 composite ceramic target을 사용하여 RF magnetron sputtering 방법으로 기판온도 약 30$0^{\circ}C$에서 RZT 박막을 Pt/Ti/Si 기판위에 증착시켰다. 안정상인 perovskite 구조를 형성시키기 위하여 PbO분위기에서 furnace annealing 과 Repid thermal annealing을 실시하여 열처리 방법에 따른 상형성 및 계면반응과 그에 따른 전기적 특성을 고찰 하였다. Pt 의 두께가 250$\AA$인 경우 furnace annealing 시 $650^{\circ}C$에서 perouskite 상이 형성되었으나 Pt층이 산소의 확산을 방지하지 못하여 상부의 Ti 층이 TiOx로 변태하였으며 하부의 Ti는 Si 과 반응하여 Ti-silicide 롤 변태하였다. 또한 75$0^{\circ}C$,60sec 인 경우 Pt 층의 응집화가 관찰되어 하부전극으로서 적용이 적절하지 못하다. 급속열처리를 실시한 경우에도 마찬가지로 Ti 층이 TiOx 와 silicide 층으로 변태되었다. Pt의 두께가 1000$\AA$인 경우에도 250$\AA$와는 달리 RTA 시 (III)방향으로 Furace annealing 시(001)방향으로 우선 성장하였다. 이는 Ti(001), P(111),PZT(111)면의 lattic mismatch 가 매우 작은데다 RTA 시 계면반응이 거의발생하지 않아 PZT 박막이 (111) 방향으로 우선 성장한 것으로 보인다. Furnace annealing 경우는 심한 계면반응이 발생하여 Pt층에 어느 정도 영향을 주었기 때문에 우선성장 방향이 바뀌었다구 생각한다.

• Proceedings of the Korean Magnestics Society Conference
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• 2011.06a
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• pp.129-129
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• 2011

The limited understanding of the surface properties of $Pt_3Ni$ for the oxygen reduction reaction (ORR) in polymer electrolyte membrane fuel cell (PEMFC) has motivated the study of properties and electronic structures of seven layered $Pt_3Ni$ (001), (110), and (111) surfaces. The first principle method based on density functional theory (DFT) is carried out. It is found that the bulk $Pt_3Ni$ has a ferromagnetic ground state with the ordered fcc type L12 structure, which is in good agreement with other results. Non magnetic Pt has the induced magnetic moment due to the strong hybridization between 3d Ni and 5d Pt. The magnetic moment of Pt and Ni enhanced on the surface of each due to surface effect however the magnetic moment of surface Pt in the Pt-segregated Pt3Ni (111) decreased and the magnetic moment of Ni in Ni rich subsurface increased significantly. The calculated d band centers of Pt explain the possibilities for oxygen absorption and play the important roles in altering the catalytic properties. The spin polarized densities of states are presented in order to understand physical properties of Pt in different surfaces in detail.

• Analytical Science and Technology
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• v.8 no.4
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• pp.723-730
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• 1995

Cyclic voltammetry and in situ STM were employed to examine the interfacial structures of a Pt(111) electrode in 0.1 mM KCN (pH9.5) and 0.1 mM KSCN (pH7) solutions. In situ STM atomic resolution revealed well ordered (2${\surd}$3${\times}$2${\surd}$3)$R30^{\circ}$-6CN and ($2{\times}2$)-2SCN structures within the double layer charging region. Six CN adsorbates formed a hollow hexagon, which embraced a coadsorbed $K^+$ cation. In contrast, the coadsorbed $K^+$ cations on the SCN covered Pt(111) were poorly ordered, despite adsorbed SCN formed a long range ordered ($2{\times}2$)-2SCN adlattice. In situ STM revealed the pronounced influence of potential in controlling the structures of compact layers at the proximity of a Pt electrode. Cathodic polarization facilitated the replacement of the coadsorbed cations by protons.

• The Korean Journal of Ceramics
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• v.6 no.3
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• pp.315-317
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• 2000

A magnetoplumbite type of Ba ferrite(BaM) layers were deposited on Pt(111) and Pt(200) layers, and their c-axis orientation and magnetic characteristics were compared each other. The as-deposited BaM layer on Pt(111) one at the substrate temperature $T_s$ above $500^{\circ}C$ revealed remarkable c-axis orientation. The saturation magnetization 4$\piM_s$ and the perpendicular coercivity $H_{c⊥}$ of the films as-deposited at $T_s$ of $600^{\circ}C$ were 4.0kG and 2.5kOe, respectively. On the other hand, BaM ferrite layer deposited on Pt(200) layer at $T_s$ as relatively low as $500^{\circ}C$ also revealed weak c-axis orientation as well as (107) one and the films as-deposited at $T_s$ of $600^{\circ}C$ exhibited 4$\piMs_{and}$ $H_{c⊥}$ of 2.8kG and 2.5kOe, respectively. It was suggested that although chemical activity of Pt surface was effective for the formation of BaM crystallites, the lattice matching was also important for obtaining BaM layer with good c-axis orientation and large perpendicular anisotropy.sotropy.

• Proceedings of the Korean Magnestics Society Conference
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• 2000.09a
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• pp.377-378
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• 2000

• Bulletin of the Korean Chemical Society
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• v.22 no.3
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• pp.267-270
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• 2001

The adsorption of chlorine on a Pt(111) surface at 90 K has been studied using scanning tunneling microscopy (STM) in ultra-high vacuum environments. The adsorbed chlorine atoms give rise to two different ordered structures, (3${\times}$3)-Cl and c(4${\times}$2)- Cl, depending on the coverage. It has been determined from the STM image that the absolute coverage of (3${\times}$3)-Cl structure is 0.44, which is not in agreement with coverage calibrated by a low energy electron diffraction technique together with an Auger electron spectrometer and a thermal desorption spectrometer. The Cl atoms bound to on-top sites at the Pt(111)(3${\times}$3)-Cl surface appeared to effectively perturb the density of states of Pt atoms, as compared with that bound to bridging sites. The other ordered structure, c(4${\times}$2)-Cl, with small domain sizes, consists of both on-top and bridge-bonded species with a saturation coverage of 0.5.

• Proceedings of the Korean Magnestics Society Conference
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• 2004.12a
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• pp.229-230
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• 2004

• Bulletin of the Korean Chemical Society
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• v.30 no.12
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• pp.2875-2876
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• 2009