• 제목/요약/키워드: film structure

검색결과 3,909건 처리시간 0.031초

밀집된 금속 나노 입자 레이어의 광학 특성 (Enhanced Light Transmittance of Densely Packed Metal Nanoparticle Layers)

  • 전현지;최진일
    • 한국재료학회지
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    • 제30권12호
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    • pp.701-708
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    • 2020
  • Irradiation of the metal nanoparticles causes local plasmon resonance in a specific wavelength band, which can improve the absorption and scattering properties of a structure. Since noble metal nanoparticles have better resonance effects than those of other metals, it is easy to identify plasmonic reactions and this is advantageous to find the optical tendency. Compared to having a particle gap or randomly arranged particle structures, densely and evenly packed structures can exhibit more uniform optical properties. Using the uniform properties, the structure can be applied to optical filtering applications. Therefore, in this paper, validation tests about metal nanoparticles and thin film structures are conducted for more accurate analysis. The optical properties of monolayer and bilayer noble metal nanoparticle structures with different diameters, packed in a uniform array, are investigated and their optical trends are analyzed. In addition, a thin film structure under identical conditions as metal nanoparticle structure is evaluated to confirm the improved optical characteristics.

Heterogeneously Integrated Thin-film Lithium Niobate Electro-optic Modulator Based on Slot Structure

  • Li, Xiaowei;Xu, Yin;Huang, Dongmei;Li, Feng;Zhang, Bo;Dong, Yue;Ni, Yi
    • Current Optics and Photonics
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    • 제6권3호
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    • pp.323-331
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    • 2022
  • Electro-optic modulator (EOM) takes a vital role in connecting the electric and optical fields. Here, we present a heterogeneously integrated EOM based on the lithium niobate-on-insulator (LNOI) platform. The key modulation waveguide structure is a field-enhanced slot waveguide formed by embedding silicon nanowires in a thin-film lithium niobate (LN), which is different from the previously reported LN ridge or etchless LN waveguides. Based on such slot structure, optical mode field area is reduced and enhanced electric field in the slot region can interact well with LN material with high Electro-optic (EO) coefficient. Therefore, the improvements in both aspects have positive effects on enhancing the modulation performance. From results, the corresponding EOM by adding such modulation waveguide structure achieves better performance, where the key half-wave-voltage-length product (V𝜋L) and 3 dB EO bandwidth are 1.78 V·cm and 40 GHz under the electrode gap width of only 6 ㎛, respectively. Moreover, Lower V𝜋L can also be achieved. With these characteristics, such field-enhanced waveguide structure could further promote the development of LNOI-based EOM.

Large Size and High Resolution Organic Light Emitting Diodes Based on the In-Ga-Zn-O Thin Film Transistors with a Coplanar Structure

  • Hong Jae Shin
    • 한국재료학회지
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    • 제33권12호
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    • pp.511-516
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    • 2023
  • Amorphous In-Ga-Zn-O (a-IGZO) thin film transistors (TFTs) with a coplanar structure were fabricated to investigate the feasibility of their potential application in large size organic light emitting diodes (OLEDs). Drain currents, used as functions of the gate voltages for the TFTs, showed the output currents had slight differences in the saturation region, just as the output currents of the etch stopper TFTs did. The maximum difference in the threshold voltages of the In-Ga-Zn-O (a-IGZO) TFTs was as small as approximately 0.57 V. After the application of a positive bias voltage stress for 50,000 s, the values of the threshold voltage of the coplanar structure TFTs were only slightly shifted, by 0.18 V, indicative of their stability. The coplanar structure TFTs were embedded in OLEDs and exhibited a maximum luminance as large as 500 nits, and their color gamut satisfied 99 % of the digital cinema initiatives, confirming their suitability for large size and high resolution OLEDs. Further, the image density of large-size OLEDs embedded with the coplanar structure TFTs was significantly enhanced compared with OLEDs embedded with conventional TFTs.

Metal-insulator Transition in $(Sr_{0.75},\;La_{0.25})TiO_3$ Ultra-thin Films

  • Choi, Jae-Du;Choi, Eui-Young;Lee, Yun-Sang;Lee, Jai-Chan
    • 한국재료학회:학술대회논문집
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    • 한국재료학회 2011년도 추계학술발표대회
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    • pp.19.2-19.2
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    • 2011
  • The $(Sr_{0.75},\;La_{0.25})TiO_3$ (SLTO) ultra-thin films with various thicknesses have been grown on Ti-O terminated $SrTiO_3$(100) substrate using Laser-Molecular Beam Epitaxy (Laser MBE). By monitoring the in-situ specular spot intensity oscillation of reflection high energy electron diffraction (RHEED), we controlled the layer-by-layer film growth. The film structure and topography were verified by atomic force microscopy (AFM) and high resolution thin film x-ray diffraction by the synchrotron x-ray radiation. We have also investigated the electronic band structure using x-ray absorption spectroscopy (XAS). The ultra thin SLTO film exhibits thickness driven metal-insulator transition around 8 unit cell thickness when the film thickness progressively reduced to 2 unit cell. The SLTO thin films with an insulating character showed band splitting in Ti $L_3-L_2$ edge XAS spectrum which is attributed to Ti 3d band splitting. This narrow d band splitting could drive the metal-insulator transition along with Anderson Localization. In optical conductivity, we have found the spectral weight transfer from coherent part to incoherent part when the film thickness was reduced. This result indicates the possibility of enhanced electron correlation in ultra thin films.

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Anodic Dissolution Property and Structure of Passive Films on Equiatomic TiNi Intermetallic Compound

  • Lee, Jeong-Ja;Yang, Won-Seog;Hwang, Woon-Suk
    • Corrosion Science and Technology
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    • 제6권6호
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    • pp.311-315
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    • 2007
  • The anodic polarization behavior of equiatomic TiNi shape memory alloy with pure titanium as a reference material was investigated by means of open circuit potential measurement and potentiodynamic polarization technique. And the structure of passive films on TiNi intermetallic compounds was also conducted using AES and ESCA. While the dissolved Ni(II) ion did not affect the dissolution rate and passivation of TiNi alloy, the dissolved Ti(III) ion was oxidated to Ti(IV) ion on passivated TiNi surface at passivation potential. It has also been found that the Ti(IV) ion increases the steady state potential, and passivates TiNi alloy at a limited concentration of Ti(IV) ion. The analysis by AES showed that passive film of TiNi alloy was composed of titanium oxide and nickel oxide, and the content of titanium was three times higher than that of nickel in outer side of passive film. According to the ESCA analysis, the passive film was composed of $TiO_2$ and NiO. It seems reasonable to suppose that NiO could act as unstabilizer to the oxide film and could be dissolved preferentially. Therefore, nickel oxide contained in the passive film may promote the dissolution of the film, and it could be explained the reason of higher pitting susceptibility of TiNi alloy than pure Ti.

Passivation Layers for Organic Thin-film-transistors

  • Lee, Ho-Nyeon;Lee, Young-Gu;Ko, Ik-Hwan;Kang, Sung-Kee;Lee, Seong-Eui;Oh, Tae-Sik
    • Transactions on Electrical and Electronic Materials
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    • 제8권1호
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    • pp.36-40
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    • 2007
  • Inorganic layers, such as SiOxNy and SiOx deposited using plasma sublimation method, were tested as passivation layer for organic thin-film-transistors (OTFTs). OTFTs with bottom-gate and bottom-contact structure were fabricated using pentacene as organic semiconductor and an organic gate insulator. SiOxNy layer gave little change in characteristics of OTFTs, but SiOx layer degraded the performance of OTFTs severely. Inferior barrier properties related to its lower film density, higher water vapor transmission rate (WVTR) and damage due to process environment of oxygen of SiOx film could explain these results. Polyurea and polyvinyl acetates (PVA) were tested as organic passivation layers also. PVA showed good properties as a buffer layer to reduce the damage come from the vacuum deposition process of upper passivation layers. From these results, a multilayer structure with upper SiOxNy film and lower PVA film is expected to be a superior passivation layer for OTFTs.

Sol-Gel 법으로 제작한 PZT이종층 박막의 운전 및 누설전류 특성 (Dielectric Properties and Leakage Current Characteristics of PZT Heterolayered Thin Films by the Sol-Gel Method)

  • 심광택;이영희;이성갑;배선기
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1997년도 하계학술대회 논문집 C
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    • pp.1229-1231
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    • 1997
  • In this work, PZT(20/80)/(80/20) heterolayered thin film that has the tetragonal and rhombohedral structure was fabricated by Sol-Gel method spin-coated on the Pt/Ti/$SiO_2$/Si substrate by turns. The thickness of PZT-1 film obtained by six-times of drying/sintering process was about 480[nm]. This procedure was repeated several times to form PZT heterolayered thim film. PZT-5 thin films with top layer of tetragonal PZT(20/80) thin film showed dense grain structure and PZT-6 thin film with top layer of rhombohedral PZT(80/20) thin film showed the microstructure without rosette. Dielectric constant increased with increasing the number of coatings, and it was about 13S5 at PZT-6 thin film. Dielectric loss was not depend on the number of coatings.

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띠 굽힘 시험을 통한 100 nm 두께 금 박막의 기계적 특성 평가 (Mechanical characterization of 100 nm-thick Au thin film using strip bending test)

  • 김재현;이학주;한승우;백창욱;김종만;김용권
    • 대한기계학회:학술대회논문집
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    • 대한기계학회 2004년도 춘계학술대회
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    • pp.252-257
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    • 2004
  • Nanometer-sized structures are being applied to many devices including micro/nano electronics, optoelectronics, quantum devices, MEMS/NEMS, biosensors, etc. Especially, the thin film with submicron thickness is a basic structure for fabricating these devices, but its mechanical behaviors are not well understood. The mechanical properties of the thin film are different from those of the bulk structure and are difficult to measure because of its handling inconvenience. Several techniques have been applied to mechanical characterization of the thin film, such as nanoindentation test, micro/nano tensile test, strip bending test, etc. In this study, we focus on the strip bending test because of its high accuracy and moderate specimen preparation efforts, and measure Au thin film, which is a very popular material in micro/nano electronic devices. Au film is deposited on Si substrate by evaporation process, of which thickness is 100nm. Using the strip bending test, we obtain elastic modulus, yield and ultimate tensile strength, and residual stress of Au thin film.

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도시 정체성과 시공간 구조의 관계 -장률(張律)의 영화 <군산: 거위를 노래하다>를 중심으로 (Relationship between Urban Identity and Time and Space - Focusing on , Zhang Lu's Film)

  • 조명기
    • 대중서사연구
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    • 제27권3호
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    • pp.151-191
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    • 2021
  • 이 글은, 영화 <군산>이 재현하는 군산 도시 정체성의 내용은 무엇이며 구성 양상은 어떠한지, 그리고 이 도시 정체성 내용과 구성양상이 영화 서사의 구조와 어떻게 호응하는지를 살핀다. <군산>은 군산과 서울을 즉자적인 도시로 전제하는 동시에 상호 영향 관계에 의해 끊임없이 재구성되는 도시로 엮어낸다. 영화 서사 시간이 종료되는 서울은 다시 군산 여행을 위한 출발지로 전환되는데, 관객이 사후적으로 회귀하는 두 곳 즉 영화 서사 시간의 시작 지점 그리고 타이틀이 제시되는 지점이다. 이 영화의 여로형 서사 구조는 2차원의 평면적 원점회귀라기보다는 3차원의 입체적 나선형이다. <군산>은 이 나선형의 시공간적 구조 위에서 두 도시의 성격 그리고 도시 정체성의 선험성에 대해 형상화한다. 서울은 거대서사·집단기억과 미시서사·개인기억의 관계를 불가지한 것으로 단절시키는 도시, 관계·기억을 단절시키고 기억의 지속을 부정하는 도시다. 반면, 군산은 거대서사·집단기억과 미시 서사·개인기억이 공존하는 도시며, 단절의식·고립의식이 치유되고 상호 위로받는 도시다. 동시에 영화는 군산을 서울의 잉여, 대타적 공간으로 재현하는 한편 군산의 정체성을 확고하고 즉자적인 것으로도 그린다. 영화는 스토리와 서사구성의 상응을 통해, 군산과 서울을 역사적 단절과 지속이 교호하는 장(場), 상호대타적인 공간인 동시에 완고한 고유성의 공간으로 이해한다. 이 글은, 도시 정체성을 구성하는 시공간적 관계성과 영화 서사의 구조가 호응하는 양상을 살폈다는 데 의의가 있다.

A study on Electronic Properties of Passive Film Formed on Ti

  • Kim, DongYung;Kwon, HyukSang
    • Corrosion Science and Technology
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    • 제2권5호
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    • pp.212-218
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    • 2003
  • Electronic properties of passive films formed on Ti at film formation potentials $(E_f)V_{SCE}$ in pH 8.5 buffer solution and in an artificial seawater were examined through the photocurrent measurement and Mott-Schottky analysis. The passive films formed on Ti in pH 8.5 buffer solution exhibited a n-type semiconductor with a band gap energys $(E_g);E_g^{n=2}=3.4$ eV for nondirect electron transition, and $E_g^{n=0.5}=3.7$ eV for direct electron transition. These band gap values were almost same as those for the passive films formed in artificial seawater, indicating that chloride ion ($Cl^-$ in solution did not affect the electronic structure of the passive film on Ti. $E_g$ for passive films formed on Ti were found to be greater than those ($E_g^{n=0.5}=3.1$ eV, $E_g^{n=2}=3.4$) for a thermal oxide film formed on Ti in air at $400^{\circ}C$. The disorder energy of passive film, determined from the absorption tail of photocurrent spectrum, was much greater than that for the thermal oxide film farmed on Ti in air at $400^{\circ}C$. The greater $E_g$ and the higher disorder energy for the passive film compared with those for the thermal oxide fIlm suggest that the passive film on Ti exhibited more disorded structure than the thermal oxide film. The donor density (about $2.4{\times}10^{20}cm^{-3}$) for the passive film formed in artificial seawater was greater than that (about $20{\times}10^{20}cm^{-3}$) formed in pH 8.5 buffer solution, indicating that $Cl^-$ increased the donor density for the passive film on Ti.