• Steel and Composite Structures
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• v.21 no.1
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• pp.1-36
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• 2016

In the present study, the nonlinear magneto-electro-mechanical free vibration behavior of rectangular double-bonded sandwich microbeams based on the modified strain gradient theory (MSGT) is investigated. It is noted that the top and bottom sandwich microbeams are considered with boron nitride nanotube reinforced composite face sheets (BNNTRC-SB) with electrical properties and carbon nanotube reinforced composite face sheets (CNTRC-SB) with magnetic fields, respectively, and also the homogenous core is used for both sandwich beams. The connections of every sandwich beam with its surrounding medium and also between them have been carried out by considering Pasternak foundations. To take size effect into account, the MSGT is introduced into the classical Timoshenko beam theory (CT) to develop a size-dependent beam model containing three additional material length scale parameters. For the CNTRC and BNNTRC face sheets of sandwich microbeams, uniform distribution (UD) and functionally graded (FG) distribution patterns of CNTs or BNNTs in four cases FG-X, FG-O, FG-A, and FG-V are employed. It is assumed that the material properties of face sheets for both sandwich beams are varied in the thickness direction and estimated through the extended rule of mixture. On the basis of the Hamilton's principle, the size-dependent nonlinear governing differential equations of motion and associated boundary conditions are derived and then discretized by using generalized differential quadrature method (GDQM). A detailed parametric study is presented to indicate the influences of electric and magnetic fields, slenderness ratio, thickness ratio of both sandwich microbeams, thickness ratio of every sandwich microbeam, dimensionless three material length scale parameters, Winkler spring modulus and various distribution types of face sheets on the first two natural frequencies of double-bonded sandwich microbeams. Furthermore, a comparison between the various beam models on the basis of the CT, modified couple stress theory (MCST), and MSGT is performed. It is illustrated that the thickness ratio of sandwich microbeams plays an important role in the vibrational behavior of the double-bonded sandwich microstructures. Meanwhile, it is concluded that by increasing H/lm, the values of first two natural frequencies tend to decrease for all amounts of the Winkler spring modulus.

• JSTS:Journal of Semiconductor Technology and Science
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• v.14 no.5
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• pp.557-565
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• 2014

We report the effect of basal-plane stacking faults (BSFs) on X-ray diffraction (XRD) of non-polar (11$\underline{2}$0) a-plane GaN films with different $SiN_x$ interlayers. Complete $SiN_x$ coverage and increased three-dimensional (3D) to two-dimensional (2D) transition stages substantially reduce BSF density. It was revealed that the Si-doping profile in the Si-doped GaN layer was unaffected by the introduction of a $SiN_x$ interlayer. The smallest in-plane anisotropy of the (11$\underline{2}$0) XRD ${\omega}$-scan widths was found in the sample with multiple $SiN_x$ layers, and this finding can be attributed to the relatively isotropic GaN mosaic resulting from the increase in the 3D-2D growth step. Williamson-Hall (WH) analysis of the (h0$\underline{h}$0) series of diffractions was employed to determine the c-axis lateral coherence length (LCL) and to estimate the mosaic tilt. The c-axis LCLs obtained from WH analyses of the present study's representative a-plane GaN samples were well correlated with the BSF-related results from both the off-axis XRD ${\omega}$-scan and transmission electron microscopy (TEM). Based on WH and TEM analyses, the trends in BSF densities were very similar, even though the BSF densities extracted from LCLs indicated that the values were reduced by a factor of about twenty.

• Journal of IKEEE
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• v.22 no.1
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• pp.205-208
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• 2018

In this work, we performed reverse- and forward-gate bias stress tests on normally-off AlGaN/GaN high electron mobility transistors(HEMTs) with p-AlGaN-gate for reliability assessment. Inverse piezoelectric effect, commonly observed in Schottky-gate AlGaN/GaN HEMTs during reverse bias stress, was not observed in p-AlGaN-gate AlGaN/GaN HEMTs. Forward gate bias stress tests revealed distinct degradation of p-AlGaN-gate devices exhibiting sudden increase of gate leakage current. We suggest that forward gate bias stress tests should be performed to define the failure criteria and assess the reliability of normally off p-AlGaN-gate GaN HEMTs.

• Proceedings of the Korean Vacuum Society Conference
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• 2016.02a
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• pp.222.2-222.2
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• 2016

트랜지스터 응용 등에 관한 연구가 활발해 지면서 에너지 밴드갭이 0 eV에 가까운 그래핀 이외의 밴드 갭 조절이 가능한 MoS2 (molybdenum disulfide), BN (boron nitride), Bi2Te3 (bismuth telluride), WS2 (tungsten disulfide) 등과 같은 이차원 Transition Metal DiChalcogenides (TMDC) 물질이 반도체 물질로 각광받고 있다. 특히 MoS2의 경우 단결정 덩어리 상태에서는 약 1.3 eV의 밴드갭을 가지나 두께가 줄어들어 두 층일 경우에는 약 1.65 eV, 단일층이 되면 약 1.9 eV의 밴드갭을 가져 박막 층수에 따라 에너지 밴드갭 조절이 가능한 것으로 알려져있다. 하지만 두께 조절이 가능하면서 대면적, 고품질을 가지는 MoS2 박막 합성은 아직 제한적이라 할 수 있으며 새로운 방법 및 물질에 대한 연구가 지속적으로 이루어 지고 있다. 따라서 본 연구에서는 다양한 층수를 지니는 MoS2 합성을 위해 나노 두께의 MoS2 박막을 CF4 plasma 를 이용하여 layer etching 진행하고 CF4 plasma 100초 etching 진행한 2 layer 두께의 MoS2를 기준으로 H2S plasma를 이용하여 treatment 진행하였다. 물리적, 화학적 분석은 Raman spectroscopy, XPS(X-ray Photoelectron Spectroscopy), AFM (Atomic Force Microscopy) 등을 이용해 진행하였고 이를 통해 MoS2 layer 감소 및 damage recovery 등을 확인하였다.

• Proceedings of the Korean Vacuum Society Conference
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• 2016.02a
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• pp.300.1-300.1
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• 2016

최근 반도체 회로의 미세화로 인해 디자인 공정이 20 nm 이하로 내려갔다. 그 결과 회로간의 간격이 줄었으며 많은 문제가 발생 한다. 첫 번째 문제는 미세하게 여러 박막 층들을 쌓기 때문에 박막 층이 그전 50 nm 공정에 비해선 쉽게 무너질 수 있다. 따라서 하나의 박막 층은 다른 여러 박막들의 하중을 잘 견뎌야 할 것이다. 결과적으로 회로의 미세화에 따라 박막의 기계적 특성이 좋아야 될 것이다. 또 다른 문제는 너무 좁은 회로의 간격으로 인해 다른 회로에 영향을 미치는 크로스토크라는 전기적 문제이다. 크로스토크가 크다는 것은 회로간의 누설 전류가 크다는 것을 의미하며 그만큼 신호 전달 능력이 감소 한다는 것을 뜻한다. 크로스토크의 문제점을 해결하기 위해 회로 사이에 절연 막을 만들어 누설전류를 막아야 한다. 이러한 문제를 바탕으로 본 연구는 Zirconium nitride (ZrN) 박막이 이러한 문제점을 해결 할 수 있는 지연구해 보았다. 박막 제작 시 변화 요인은 질소유량 과 열처리 온도 이며 질소유량 변화는 2 sccm 과 8 sccm 두 경우로 하였다. 또한 열처리는 As-deposited state, $600^{\circ}C$ 와 $800^{\circ}C$로 열처리 하였다. 박막 증착은 RF magnetron sputtering을 이용하였으며 열처리는 질소 분위기에서 furnace를 이용하였다. 기계적 특성분석 결과 질소유량이 2 sccm 인 박막의 hardness는 as-deposited stste에서 18.8 GPa이고 $600^{\circ}C$에선 18.4 GPa로 거의 비슷하고 $800^{\circ}C$ 열처리한 경우는 15.4 GPa 으로 hardness가 감소하는 것을 알 수 있었다. 질소 유량을 8 sccm 흘려주며 증착한 박막의 경우는 as-deposited state, $600^{\circ}C$, $800^{\circ}C$에서의 hardness가 각각 17.5, 16.4, 21.1 GPa 으로 감소하다가 증가하는 경향을 보였다. 또한 zrN 박막의 전기적 특성인 누설 전류 밀도도 측정하였다. 결과적으로 본 연구는 ZrN 박막의 질소 유량 변화와 열처리에 따른 기계적, 전기적 특성변화를 확인 하였다.

• Journal of Sensor Science and Technology
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• v.23 no.6
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• pp.420-424
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• 2014

Aluminum-scandium nitride ($Al_{1-x}Sc_xN$) thin films with a TiN buffer layer have been fabricated on SUS430 substrate by RF reactive magnetron sputtering at room temperature under 50% $N_2$/Ar. The effect of Sc-doping on the structure and piezoelectric properties of AlN films has been investigated using SEM, XRD, surface profiler and pressure-voltage measurements. The as-deposited AlN films showed polycrystalline phase, and the Sc-doped AlN film, the peak of AlN (002) plane and the crystallinity became very strong. With Sc-doping, the crystal size of AlN film was grown from ~20 nm to ~100 nm. The output signal voltage of AlN sensor showed a linear behavior between 15~65 mV, and output signal voltage of Sc-doped AlN sensor was increased over 7 times. The pressure-sensing sensitivity of AlN film was calculated about 10.6mV/MPa, and $Al_{0.88}Sc_{0.12}N$ film was calculated about 76 mV/MPa.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.25 no.6
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• pp.231-238
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• 2015

Sapphire single crystals have been highlighted for epitaxial of gallium nitride films in high-power laser and light emitting diode industries. Among the many crystal growth methods, vertical Bridgman process is an excellent commercial method for growing high quality sapphire crystals with c-axis. In this study, the thermally induced stress in Sapphire during the vertical Bridgman crystal growth process was investigated using a finite element model. A vertical Bridgman process of 2-inch Sapphire was considered for the model. The effects of vertical and transverse temperature gradients on the thermal stress during the process were discussed based on the finite element analysis results.

• Proceedings of the Korean Vacuum Society Conference
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• 2015.08a
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• pp.189-189
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• 2015

Plasmonics, sensor, field effect transistors, solar cells 등 다양한 적용분야를 가지는 실리콘 구조체는 제작공정에 의해 전기적 및 광학적 특성이 달라지기 때문에 적합한 나노구조 제작방법이 요구되고 있다. 나노구조체 제작방법으로는 Photo lithography, Extreme ultraviolet lithography (EUV), Nano imprinting lithography (NIL), Block copolymer (BCP) 방식의 방법들이 연구되고 있으며, 특히 BCP는 direct self-assembly 특성을 가지고 있으며 가격적인 면에서도 큰 장점을 가진다. 하지만 BCP를 mask로 사용하여 식각공정을 진행할 경우 BCP가 버티지 못하고 변형되어 mask로서의 역할을 하지 못한다. 이러한 문제를 해결하기 위하여 본 논문에서는 BCP와 질화막을 이용한 double mask 방법을 사용하였다. 기판 위에 BCP를 self-assembly 시키고 mask로 사용하여 hole 부분으로 노출된 기판을 Ion gun을 통해 질화 시킨 후에 BCP를 제거한다. 기판 위에 hole 모양의 질화막 표면은 BCP와 다르게 etching 공정 중 변형되지 않는다. 이러한 질화막 표면을 mask로 사용하여 pillar pattern의 실리콘 나노구조체를 제작하였다. 질화막 mask로 사용되는 template은 PS와 PMMA로 구성된 BCP를 사용하였다. 140kg/mol의 polystyrene과 65kg/mol의 PMMA를 톨루엔으로 용해시키고 실리콘 표면 위에 spin coating으로 도포하였다. Spin coat 후 230도에서 40시간 동안 열처리를 진행하여 40nm의 직경을 가진 PS-b-PMMA self-assembled hole morphology를 형성하였다. 질화막 형성 및 etching을 위한 장비로 low-energy Ion beam system을 사용하였다. Reactive Ion beam은 ICP와 3-grid system으로 구성된 Ion gun으로부터 형성된다. Ion gun에 13.56 MHz의 frequency를 갖는 200W 전력을 인가하였다. Plasma로부터 나오는 Ion은 $2{\Phi}$의 직경의 hole을 가지는 3-grid hole로 추출된다. 10~70 voltage 범위의 전위를 plasma source 바로 아래의 1st gird에 인가하고, 플럭스 조절을 위해 -150V의 전위를 2nd grid에 인가한다. 그리고 3rd grid는 접지를 시켰다. chamber내의 질화 및 식각가스 공급은 2mTorr로 유지시켰다. 그리고 기판의 온도는 냉각칠러를 이용하여 -20도로 냉각을 진행하였다. 이와 같은 공정 결과로 100 nm 이상의 높이를 갖는 40 nm직경의 균일한 Silicon pillar pattern을 형성 할 수 있었다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2009.06a
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• pp.235-235
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• 2009

This paper describes the influence of a polycrystalline (poly) 3C-SiC buffer layer on the surface acoustic wave (SAW) properties of poly aluminum nitride (AlN) thin films by comparing the center frequency, insertion loss, the electromechanical coupling coefficient ($k^2$), andthetemperaturecoefficientoffrequency(TCF) of an IDT/AlN/3C-SiC structure with those of an IDT/AlN/Si structure, The poly-AlN thin films with an (0002)-preferred orientation were deposited on a silicon (Si) substrate using a pulsed reactive magnetron sputtering system. Results show that the insertion loss (21.92 dB) and TCF (-18 ppm/$^{\circ}C$) of the IDT/AlN/3C-SiC structure were improved by a closely matched coefficient of thermal expansion (CTE) and small lattice mismatch (1 %) between the AlN and 3C-SiC. However, a drawback is that the $k^2(0.79%)$ and SAW velocity(5020m/s) of the AlN/3C-SiC SAW device were reduced by appearing in some non-(0002)AlN planes such as the (10 $\bar{1}$ 2) and (10 $\bar{1}$ 3) AlN planes in the AlN/SiC film. Although disadvantages were shown to exist, the use of the AlN/3C-SiC structure for SAW applications at high temperatures is possible. The characteristics of the AlN thin films were also evaluated using FT-IR spectra, XRD, and AFM images.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2009.06a
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• pp.74-74
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• 2009

Titanium nitride has been used as hardmask for semiconductor process, capacitor of MIM type and diffusion barrier of DRAM, due to it's low resistivity, thermodynamic stability and diffusion coefficient. Characteristics of the TiN film are high intensity and chemical stability. The TiN film also has compatibility with high-k material. This study is an experimental test for better condition of TiN film etching process. The etch rate of TiN film was investigated about etching in $BCl_3/Ar/O_2$ plasma using the inductively coupled plasma (ICP) etching system. The base condition were 4 sccm $BCl_3$ /16 sccm Ar mixed gas and 500 W the RF power, -50 V the DC bias voltage, 10 mTorr the chamber pressure and $40\;^{\circ}C$ the substrate temperature. We added $O_2$ gas to give affect etch rate because $O_2$ reacts with photoresist easily. We had changed $O_2$ gas flow rate from 2 sccm to 8 sccm, the RF power from 500 W to 800 W, the DC bias voltage from -50 V to -200 V, the chamber pressure from 5 mTorr to 20 mTorr and the substrate temperature from $20\;^{\circ}C$ to $80\;^{\circ}C$.