• Title/Summary/Keyword: SPM(Scanning Probe Microscopy)

Search Result 42, Processing Time 0.026 seconds

T-OLED의 반사전극으로 사용하기 위한 Ag 박막 표면의 UV에 의한 산화 및 KPFM을 이용한 표면 전위 측정

  • Kim, Seong-Jun;Kim, Su-In;Kim, Dong-Uk;Kim, Ju-Yeon;Lee, Eun-Hyeok;Sin, Dong-Hun;Lee, Chang-U
    • Proceedings of the Korean Vacuum Society Conference
    • /
    • 2013.08a
    • /
    • pp.182.1-182.1
    • /
    • 2013
  • Silver (Ag)는 높은 반사율을 가지고 있어 Top-Emission Organic Light Emitting Diode (T-OLED)의 반사전극으로 사용하기 적합하지만 일함수가 낮은 단점 (4.3 eV)을 가지고 있다. 이런 낮은 일함수를 증가시키기 위하여 Ag 박막 표면을 산화시켜 일함수를 증가시키기 위한 연구가 진행중에 있으며, 이 연구에서는 UV로 $O_3$을 발생시켜 Ag 박막 표면을 산화시키기 위한 연구를 진행하였다. 특히, Ag 박막 표면의 일함수 변화를 측정하기 위하여 SPM (Scanning Probe Microscopy)의 KPFM (Kelvin Probe Force Microscopy) mode를 적용하여 nano 영역에서의 일함수 변화를 surface potential로 측정하여 UV 표면 산화에 의한 표면 일함수 형상을 확인하였다. Ag 박막은 rf magnetron sputter를 사용하여, Si 기판위에 300nm 두께로 증착시켰다. 이후 $O_3$ 발생되는 UV 램프로 Ag 박막 표면 30초 간격으로 최대 5분간 산화시켰으며, 이후 KPFM mode를 사용하여 산화 시간에 따른 Ag 박막 표면의 potential 변화를 측정하였다. 0~3분간 산화된 Ag 박막 표면의 potential은 약 6 mV로 일정하였으나 3분 이후 최대 110 mV까지 급격하게 변화하는 것을 확인할 수 있었다. Ag 박막 표면의 RMS roughness는 UV 산화처리 전0.7 nm였으나, potential이 급격하게 증가하는 시점인 3분 이후 2.83 nm로 약 400% 이상 증가하였다. 이를 통해 $O_3$ 발생 UV 램프로 산화된 Ag 박막의 표면 물성은 처리 시간에 따라 급격히 변하는 것을 확인하였다.

  • PDF

Simultaneous Formation of NiSi Contact and Cu Plug/Ti Barrier (NiSi 접촉과 Cu 플러그/Ti 확산방지층의 동시 형성 연구)

  • Bae, Kyoo-Sik
    • Korean Journal of Materials Research
    • /
    • v.20 no.6
    • /
    • pp.338-343
    • /
    • 2010
  • As an alternative to the W plug used in MOSFETs, a Cu plug with a NiSi contact using Ta / TaN as a diffusion barrier is currently being considered. Conventionally, Ni was first deposited and then NiSi was formed, followed by the barrier and Cu deposition. In this study, Ti was employed as a barrier material and simultaneous formation of the NiSi contact and Cu plug / Ti barrier was attempted. Cu(100 nm) / Ti / Ni(20 nm) with varying Ti thicknesses were deposited on a Si substrate and annealed at $4000^{\circ}C$ for 30 min. For comparison, Cu/Ti/NiSi thin films were also formed by the conventional method. Optical Microscopy (OM), Scanning Probe Microscopy (SPM), X-Ray Diffractometry (XRD), and Auger Electron Microscopy (AES) analysis were performed to characterize the inter-diffusion properties. For a Ti interlayer thicker than 50 nm, the NiSi formation was incomplete, although Cu diffusion was inhibited by the Ti barrier. For a Ti thickness of 20 nm and less, an almost stoichiometric NiSi contact along with the Cu plug and Ti barrier layers was formed. The results were comparable to that formed by the conventional method and showed that this alternative process has potential as a formation process for the Cu plug/Ti barrier/NiSi contact system.

Atomic Force Microscopy(AFM) based Single Cell Manipulation and High Efficient Gene Delivery Technology (원자간력 현미경을 이용한 단일세포 조작 및 고효율 유전자 도입기술)

  • Han, Sung-Woong;Nakamura, Chikashi;Miyake, Jun;Kim, Woo-Sik;Kim, Jong-Min;Chang, Sang-Mok
    • Korean Chemical Engineering Research
    • /
    • v.47 no.5
    • /
    • pp.538-545
    • /
    • 2009
  • The principle and application of a scanning probe microscopy(SPM) are reviewed briefly, and a low-invasive single cell manipulation and a gene delivery technique using an etched atomic force microscopy(AFM) probe tip, which we call a nanoneedle, are explained in detail. The nanoneedle insertion into a cell can be judged by a sudden drop of force in a force-distance curve. The probabilities of nanoneedle insertion into cells were 80~90%, which were higher than those of typical microinjection capillaries. When the diameter of the nanoneedle was smaller than 400 nm, the nanoneedle insertion into a cell over 1 hour had almost no influence on the cell viability. A highly efficient gene delivery and a high ratio of expressed gene per delivered DNA compared the conventional major nonviral gene delivery methods could be achieved using the gene modified nanoneedle.

Surface Physical Properties of W-N Nano Thin Films by Nanotribological Analysis (나노트라이볼로지 분석을 이용한 W-N 나노박막의 표면 물성 연구)

  • Kim, Soo-In;Lee, Kyu-Young;Kim, Joo-Young;Lee, Chang-Woo
    • Journal of the Korean Vacuum Society
    • /
    • v.20 no.6
    • /
    • pp.456-460
    • /
    • 2011
  • Recently, the size of currently-researched components and devices reduces nano-scale. Thus, it is important and emphasizes the analyses of physical properties in nano scale. Especially, the mechanical properties are not over micro-scale components but nano-scale components with different characteristics that has been reported. However, most analytical methods for currently studying in nano-scale are related to spectroscopy and electronics, affected the limitation of viewing size that these methods give only average information. In this research, the representative nanotribology analyses, nano-indenter study the physical and mechanical properties of W-N thin film for nano region and nano depth within nano-scale that the thickness of W-N diffusion barrier has less than tens of nanometers. The Scanning probe microscopy (SPM) study the surface image. From these results, the hardness of W-N thin film underneath the nano-surface decreased from 57.67 GPa to 9.1 GPa according to the increase of nitrogen gas flow. The elastic modulus of W-N thin film underneath the nano-surface also decreased from 575.53 GPa to 178.1 GPa.

Effect of Ti Interlayer Thickness on Epitaxial Growth of Cobalt Silicides (중간층 Ti 두께에 따른 CoSi2의 에피텍시 성장)

  • Choeng, Seong-Hwee;Song, Oh-Sung
    • Korean Journal of Materials Research
    • /
    • v.13 no.2
    • /
    • pp.88-93
    • /
    • 2003
  • Co/Ti bilayer structure in Co salicide process helps to the improvement of device speed by lowering contact resistance due to the epitaxial growth of $CoSi_2$layers. We investigated the epitaxial growth and interfacial mass transport of $CoSi_2$layers formed from $150 \AA$-Co/Ti structure with two step rapid thermal annealing (RTA). The thicknesses of Ti layers were varied from 20 $\AA$ to 100 $\AA$. After we confirmed the appropriate deposition of Ti film even below $100\AA$-thick, we investigated the cross sectional microstructure, surface roughness, eptiaxial growth, and mass transportation of$ CoSi_2$films formed from various Ti thickness with a cross sectional transmission electron microscopy XTEM), scanning probe microscopy (SPM), X-ray diffractometery (XRD), and Auger electron depth profiling, respectively. We found that all Ti interlayer led to$ CoSi_2$epitaxial growth, while $20 \AA$-thick Ti caused imperfect epitaxy. Ti interlayer also caused Co-Ti-Si compounds on top of $CoSi_2$, which were very hard to remove selectively. Our result implied that we need to employ appropriate Ti thickness to enhance the epitaxial growth as well as to lessen Co-Ti-Si compound formation.

Pitch Measurement of One-dimensional Gratings Using a Metrological Atomic Force Microscope and Uncertainty Evaluation (미터 소급성을 갖는 원자간력 현미경을 이용한 1차원 격자 피치 측정과 불확도 평가)

  • Kim Jong-Ahn;Kim Jae Wan;Park Byong Chon;Eom Tae Bong;Kang Chu-Shik
    • Journal of the Korean Society for Precision Engineering
    • /
    • v.22 no.4
    • /
    • pp.84-91
    • /
    • 2005
  • We measured the pitch of one-dimensional (ID) grating specimens using a metrological atomic force microscope (M-AFM). The ID grating specimens a.e often used as a magnification standard in nano-metrology, such as scanning probe microscopy (SPM) and scanning electron microscopy (SEM). Thus, we need to certify the pitch of grating specimens fur the meter-traceability in nano-metrology. To this end, an M-AFM was setup at KRISS. The M-AFM consists of a commercial AFM head module, a two-axis flexure hinge type nanoscanner with built-in capacitive sensors, and a two-axis heterodyne interferometer to establish the meter-traceability directly. Two kinds of ID grating specimens, each with the nominal pitch of 288 nm and 700 nm, were measured. The uncertainty in pitch measurement was evaluated according to Guide to the Expression of Uncertainty in Measurement. The pitch was calculated from 9 line scan profiles obtained at different positions with 100 ㎛ scan range. The expanded uncertainties (k = 2) in pitch measurement were 0.10 nm and 0.30 nm for the specimens with the nominal pitch of 288 nm and 700 nm. The measured pitch values were compared with those obtained using an optical diffractometer, and agreed within the range of the expanded uncertainty of pitch measurement. We also discussed the effect of averaging in the measurement of mean pitch using M-AFM and main components of uncertainty.

Passivation Layer (Thermosetting Film)가 형성된 유기박막 트랜지스터의전기적 특성 변화에 대한 연구

  • Seong, Si-Hyeon;Kim, Gyo-Hyeok;Jeong, Il-Seop
    • Proceedings of the Korean Vacuum Society Conference
    • /
    • 2013.02a
    • /
    • pp.380-380
    • /
    • 2013
  • 본 논문에서는 외기 환경 요인 중에서 H2O와 O2의 영향으로 성능이 저하되는 유기박막트랜지스터(OTFT)의 수명시간 향상을 위하여 필요한 passivation layer의 효과에 대하여 알아 보았다. OTFT에 기존의 액상 공정이나 증착 공정으로 단일 passivation layer또는 다층 passivation layer를 형성하는 방식과는 다르게 향후에 산업 전반에 적용이 기대되는 것을 고려하여 제작 공정의 간편성을 위하여 film 형태로 되어 있는 열경화성 epoxy resin film으로 passivation layer를 구현하는 방법을 사용하여 OTFT의 storage stability를 평가하였다. passivation layer가 없는 OTFT와 열경화성 epoxy resin film으로 passivation된 OTFT의 전기적 특성이 서로 비교 평가되었으며 또한 30일 동안 온도 $25^{\circ}C$ 상대습도 40%의 환경을 갖는 Desicator 안에서 소자를 보관하여 시간에 따른 전기적 특성 변화를 검증하여 epoxy resin film의 passivation layer으로의 적용가능성을 검증하였다. 결과적으로 30일 후의 passivation layer가 없는 OTFT의 전기적 특성은 매우 낮게 떨어진 반면에 epoxy resin film으로 passivation layer가 구현된 OTFT의 mobility는 $0.060cm^2$/Vs, VT는 -0.18 V, on/off ratio는 $3.7{\times}10^3$으로 초기의 소자 특성이 잘 유지되는 결과를 얻었다. OTFT는 Flexible한 polyethersulfone (PES)기판에 게이트 전극이 하부에 있는 Bottom gate 구조로 제작되었고 채널 형성을 위한 유기반도체 재료로 6,13-bis (triisopropylsilylethynyl) (TIPS) pentacene이 사용되었고 spin coating된 Poly-4-vinylphenol (PVP)가 게이트 절연체로 사용되었다. 이때 Au전극은 Shadow mask를 이용하여 증착하였다. 또한 OTFT의 채널 길이 $100{\mu}m$, 채널 폭 $300{\mu}m$의 영역에 Drop casting법을 사용하여 채널을 형성하였다. 물리적 특성은 scanning electron microscopy (SEM), scanning probe microscopy (SPM), x-ray diffraction (XRD)를 사용하여 분석하였고, 전기적 특성은 Keithley-4200을 사용하여 추출하였다.

  • PDF

Electrical and Morphology Properties of Self-Assembled Dendrimer on Au (111) Substrate (Au (111)기판에 자기조립된 덴드리머 분자의 형태와 전기적 특성에 관한 연구)

  • Jung, Kyung-Han;Shin, Hoon-Kyu;Kim, Chung-Kyun;Kwon, Young-Soo
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
    • /
    • 2003.05c
    • /
    • pp.120-123
    • /
    • 2003
  • To investigate the characteristics of the single dendrimer molecule, we attempt to measure morphology and electrical properties of the self-assembled dendrimer on Au (111)substrate with SPM(scanning probe microscopy). The same self-assembly procedure was used for two different concentrations, $10{\mu}mol/ml$ and $100{\mu}mol/ml$. The case of lower concentration, we can measure the diameter and the height of the single molecule with the tapping mode AFM image. The imaged single molecules were dome shaped and the average diameter and height were 15.6 nm, 1.2 nm respectively. From these sizes, we can calculate the volume of the single molecule. The volume of the single molecule was estimated about $116nm^3$. However, that of higher concentration, it is difficult to obtain obvious image of the single molecule. To add to, I-V characteristics were investigated using STM, on which the phenomenon of negative differential resistance (NDR)was observed between 0.14 V and 0.24 V reproductively.

  • PDF

Property of Nickel Silicide with 60 nm and 20 nm Hydrogenated Amorphous Silicon Prepared by Low Temperature Process (60 nm 와 20 nm 두께의 수소화된 비정질 실리콘에 따른 저온 니켈실리사이드의 물성 변화)

  • Kim, Joung-Ryul;Park, Jong-Sung;Choi, Young-Youn;Song, Oh-Sung
    • Journal of the Korean Vacuum Society
    • /
    • v.17 no.6
    • /
    • pp.528-537
    • /
    • 2008
  • 60 nm and 20 nm thick hydrogenated amorphous silicon(a-Si:H) layers were deposited on 200 nm $SiO_2$/single-Si substrates by inductively coupled plasma chemical vapor deposition(ICP-CVD). Subsequently, 30 nm-Ni layers were deposited by an e-beam evaporator. Finally, 30 nm-Ni/(60 nm and 20 nm) a-Si:H/200 nm-$SiO_2$/single-Si structures were prepared. The prepared samples were annealed by rapid thermal annealing(RTA) from $200^{\circ}C$ to $500^{\circ}C$ in $50^{\circ}C$ increments for 40 sec. A four-point tester, high resolution X-ray diffraction(HRXRD), field emission scanning electron microscopy(FE-SEM), transmission electron microscopy(TEM), and scanning probe microscopy(SPM) were used to examine the sheet resistance, phase transformation, in-plane microstructure, cross-sectional microstructure, and surface roughness, respectively. The nickel silicide from the 60 nm a-Si:H substrate showed low sheet resistance from $400^{\circ}C$ which is compatible for low temperature processing. The nickel silicide from 20 nm a-Si:H substrate showed low resistance from $300^{\circ}C$. Through HRXRD analysis, the phase transformation occurred with silicidation temperature without a-Si:H layer thickness dependence. With the result of FE-SEM and TEM, the nickel silicides from 60 nm a-Si:H substrate showed the microstructure of 60 nm-thick silicide layers with the residual silicon regime, while the ones from 20 nm a-Si:H formed 20 nm-thick uniform silicide layers. In case of SPM, the RMS value of nickel silicide layers increased as the silicidation temperature increased. Especially, the nickel silicide from 20 nm a-Si:H substrate showed the lowest RMS value of 0.75 at $300^{\circ}C$.

Property of Nickel Silicides with Hydrogenated Amorphous Silicon Thickness Prepared by Low Temperature Process (나노급 수소화된 비정질 실리콘층 두께에 따른 저온형성 니켈실리사이드의 물성 연구)

  • Kim, Jongryul;Choi, Youngyoun;Park, Jongsung;Song, Ohsung
    • Korean Journal of Metals and Materials
    • /
    • v.46 no.11
    • /
    • pp.762-769
    • /
    • 2008
  • Hydrogenated amorphous silicon(a-Si : H) layers, 120 nm and 50 nm in thickness, were deposited on 200 $nm-SiO_2$/single-Si substrates by inductively coupled plasma chemical vapor deposition(ICP-CVD). Subsequently, 30 nm-Ni layers were deposited by E-beam evaporation. Finally, 30 nm-Ni/120 nm a-Si : H/200 $nm-SiO_2$/single-Si and 30 nm-Ni/50 nm a-Si:H/200 $nm-SiO_2$/single-Si were prepared. The prepared samples were annealed by rapid thermal annealing(RTA) from $200^{\circ}C$ to $500^{\circ}C$ in $50^{\circ}C$ increments for 30 minute. A four-point tester, high resolution X-ray diffraction(HRXRD), field emission scanning electron microscopy (FE-SEM), transmission electron microscopy (TEM), and scanning probe microscopy(SPM) were used to examine the sheet resistance, phase transformation, in-plane microstructure, cross-sectional microstructure, and surface roughness, respectively. The nickel silicide on the 120 nm a-Si:H substrate showed high sheet resistance($470{\Omega}/{\Box}$) at T(temperature) < $450^{\circ}C$ and low sheet resistance ($70{\Omega}/{\Box}$) at T > $450^{\circ}C$. The high and low resistive regions contained ${\zeta}-Ni_2Si$ and NiSi, respectively. In case of microstructure showed mixed phase of nickel silicide and a-Si:H on the residual a-Si:H layer at T < $450^{\circ}C$ but no mixed phase and a residual a-Si:H layer at T > $450^{\circ}C$. The surface roughness matched the phase transformation according to the silicidation temperature. The nickel silicide on the 50 nm a-Si:H substrate had high sheet resistance(${\sim}1k{\Omega}/{\Box}$) at T < $400^{\circ}C$ and low sheet resistance ($100{\Omega}/{\Box}$) at T > $400^{\circ}C$. This was attributed to the formation of ${\delta}-Ni_2Si$ at T > $400^{\circ}C$ regardless of the siliciation temperature. An examination of the microstructure showed a region of nickel silicide at T < $400^{\circ}C$ that consisted of a mixed phase of nickel silicide and a-Si:H without a residual a-Si:H layer. The region at T > $400^{\circ}C$ showed crystalline nickel silicide without a mixed phase. The surface roughness remained constant regardless of the silicidation temperature. Our results suggest that a 50 nm a-Si:H nickel silicide layer is advantageous of the active layer of a thin film transistor(TFT) when applying a nano-thick layer with a constant sheet resistance, surface roughness, and ${\delta}-Ni_2Si$ temperatures > $400^{\circ}C$.