• 제목/요약/키워드: Field Effect Mobility

검색결과 517건 처리시간 0.034초

AlGaN/GaN HEMT의 채널폭 스케일링에 따른 협폭효과 (Narrow channel effect on the electrical characteristics of AlGaN/GaN HEMT)

  • 임진홍;김정진;심규환;양전욱
    • 전기전자학회논문지
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    • 제17권1호
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    • pp.71-76
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    • 2013
  • 본 연구에서는 AlGaN/GaN HEMT (High electron mobility transistor)를 제작하고 채널폭의 감소에 따른 특성의 변화를 고찰하였다. AlGaN/GaN 이종접합구조 기반의 기판 위에 채널의 길이는 $1{\mu}m$, 채널 폭은 각각 $0.5{\sim}9{\mu}m$가 되도록 전자선 리소그라피 방법으로 트랜지스터를 제작하였다. 게이트를 형성하지 않은 상태에서 채널의 면저항을 측정한 결과 sub-${\mu}m$ 크기로 채널폭이 작아짐에 따라 채널의 면저항이 급격히 증가하였으며, 트랜지스터의 문턱전압은 $1.6{\mu}m$$9{\mu}m$의 채널폭에서 -2.85 V 이었으며 $0.9{\mu}m$의 채널폭에서 50 mV의 변화, $0.5{\mu}m$에서는 350 mV로 더욱 큰 변화를 보였다. 트랜스컨덕턴스는 250 mS/mm 내외의 값으로부터 sub-${\mu}m$ 채널에서 150 mS/mm로 채널폭에 따라 감소하였다. 또한, 게이트의 역방향 누설전류는 채널폭에 따라 감소하였으나 sub-${\mu}m$ 크기에서는 감소가 둔화되었는데 채널폭이 작아짐에 따라 나타는 이와 같은 일련의 현상들은 AlGaN 층의 strain 감소로 인한 압전분극 감소가 원인이 되는 것으로 사료된다.

인산질 비료에 의한 안정화 적용 토양 내 비소의 지구화학적 거동 변화 (The Alterations of Geochemical Behavior of Arsenic in Stabilized Soil by the Addition of Phosphate Fertilizer)

  • 전용중;김범준;고주인;고명수
    • 자원환경지질
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    • 제55권2호
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    • pp.209-217
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    • 2022
  • 경작을 위해 토양에 공급하는 인산질 비료가 석회석을 이용한 안정화 적용 토양에서 비소의 용출에 미치는 영향을 회분식 실험과 칼럼실험을 통해 확인하였다. 토양은 폐석탄광인 옥동, 부국 탄광 주변 경작지에서 채취하였으며, 채취한 토양의 평균 비소 농도는 20.0 mg/kg으로 나타났다. 연속추출을 통해 비소의 지구화학적 이동성이 상대적으로 높은 토양을 선택하여 실험에 사용하였다. 석회석(3 wt%)과 토양을 혼합하여 안정화 적용 토양을 준비하고 농촌진흥청에서 제시한 경작지 토양 내 유효인산 기준을 바탕으로 인산질 비료(NH4H2PO4)를 토양과 혼합하였다. 이때, 석회석과 혼합하지 않은 비교토양을 준비하여 대조군으로 활용하였다. 토양으로부터 용출되는 비소의 농도는 인산질 비료의 공급량과 양의 상관관계를 나타냈다. 이러한 결과는 안정화 유무에 따라 큰 차이를 보이지 않았다. 용출액 내 인산염(PO43-)의 농도는 석회석을 혼합한 조건에서 상대적으로 낮은 결과를 보였는데, 이러한 결과는 PO43-와 석회석에서 용해된 칼슘 이온(Ca2+)의 결합침전에 의한 것으로 판단된다. 지속적으로 관개 수를 공급하는 경작환경에서 인산질 비료가 비소의 용출에 미치는 영향을 확인하기 위해 칼럼실험을 진행하였다. 칼럼실험 초기 10 P.V.까지는 토양으로부터 비소의 용출량이 석회석 혼합조건에서 더 적었지만 이후에는 석회석 혼합조건과 상관없이 유출 수의 비소 농도가 점차 증가하였다. 칼럼실험 이후 잔류토양을 건조시켜 연속추출을 실시한 결과 안정화 조건에 상관없이 실험 전 토양과 비교하여 상대적으로 이동 가능한 형태의 비소의 분율이 증가하였다. 이러한 결과는 석회석을 이용하여 토양 안정화 공법을 적용하여도 경작과정에서 공급하는 인산질 비료에 의해 토양 내 비소의 지구화학적 이동도가 증가하여 안정화 효과가 감소할 수 있음을 보여준다.

스트레인드 채널이 무캐패시터 메모리 셀의 메모리 마진에 미치는 영향 (Impact of strained channel on the memory margin of Cap-less memory cell)

  • 이충현;김성제;김태현;오정미;최기령;심태헌;박재근
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2009년도 하계학술대회 논문집
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    • pp.153-153
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    • 2009
  • We investigated the dependence of the memory margin of the Cap-less memory cell on the strain of top silicon channel layer and also compared kink effect of strained Cap-less memory cell with the conventional Cap-less memory cell. For comparison of the characteristic of the memory margin of Cap-less memory cell on the strain channel layer, Cap-less transistors were fabricated on fully depleted strained silicon-on-insulator of 0.73-% tensile strain and conventional silicon-on-insulator substrate. The thickness of channel layer was fabricated as 40 nm to obtain optimal memory margin. We obtained the enhancement of 2.12 times in the memory margin of Cap-less memory cell on strained-silicon-on-insulator substrate, compared with a conventional SOI substrate. In particular, much higher D1 current of Cap-less memory cell was observed, resulted from a higher drain conductance of 2.65 times at the kink region, induced by the 1.7 times higher electron mobility in the strain channel than the conventional Cap-less memory cell at the effective field of 0.3MV/cm. Enhancement of memory margin supports the strained Cap-less memory cell can be promising substrate structures to improve the characteristics of Cap-less memory cell.

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Mixed-mode simulation을 이용한 4H-SiC DMOSFETs의 채널 길이에 따른 transient 특성 분석 (Mixed-mode simulation of transient characteristics of 4H-SiC DMOSFETs)

  • 강민석;최창용;방욱;김상철;김남균;구상모
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2009년도 하계학술대회 논문집
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    • pp.131-131
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    • 2009
  • Silicon Carbide (SiC) is a material with a wide bandgap (3.26eV), a high critical electric field (~2.3MV/cm), a and a high bulk electron mobility ($\sim900cm^2/Vs$). These electronic properties allow high breakdown voltage, high-speed switching capability, and high temperature operation compared to Si devices. Although various SiC DMOSFET structures have been reported so far for optimizing performances, the effect of channel dimension on the switching performance of SiC DMOSFETs has not been extensively examined. This paper studies different channel dimensons ($L_{CH}$ : $0.5{\mu}m$, $1\;{\mu}m$, $1.5\;{\mu}m$) and their effect on the the device transient characteristics. The key design parameters for SiC DMOSFETs have been optimized and a physics-based two-dimensional (2-D) mixed device and circuit simulator by Silvaco Inc. has been used to understand the relationship. with the switching characteristics. To investigate transient characteristic of the device, mixed-mode simulation has been performed, where the solution of the basic transport equations for the 2-D device structures is directly embedded into the solution procedure for the circuit equations. We observe an increase in the turn-on and turn-off time with increasing the channel length. The switching time in 4H-SiC DMOSFETs have been found to be seriously affected by the various intrinsic parasitic components, such as gate-source capacitance and channel resistance. The intrinsic parasitic components relate to the delay time required for the carrier transit from source to drain. Therefore, improvement of switching speed in 4H-SiC DMOSFETs is essential to reduce the gate-source capacitance and channel resistance.

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Hot Wall Epitaxy(HWE)법에 의한 $CulnSe_2$ 박막 성장과 특성 (Growth and Characterization of $CulnSe_2$ Single Crystal Thin Film by Hot Wall Epitaxy)

  • 홍광준;이상열;박진성
    • 한국전기전자재료학회논문지
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    • 제14권6호
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    • pp.445-454
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    • 2001
  • The stochiometric mix of evaporating materials for the CuInSe$_2$ single crystal thin films was prepared from horizontal furnace. To obtain the single crystal thin films, CuInSe$_2$ mixed crystal was deposited on thoroughly etched semi-insulating GaAs(100) substrate by the Hot Wall Epitaxy(HWE) system. The source and substrate temperature were 62$0^{\circ}C$ and 41$0^{\circ}C$, respectively. The crystalline structure of single crystal thin films was investigated by the photoluminescence and double crystal X-ray diffraction (DCXD). The carrier density and mobility of CuInSe$_2$ single crystal thin films measured from Hall effect fby van der Pauw method are 9.62x10$^{16}$ cm$^{-3}$ , 296$\textrm{cm}^2$/V.s at 293 K, respectively. From the photocurrent spectrum by illumination of perpendicular light on the c-axis of the CuInSe$_2$ single crystal thin film we have found that he values of spin orbit splitting ΔSo and the crystal field splitting ΔCr were 6.1 meV and 175.2 meV at 10K, respectively. From the photoluminescence measurement on CuInSe$_2$ single crystal thin film we observed free excition (Ex) existing only high quality crystal and neutral bound exiciton (D$^{\circ}$,X) having very strong peak intensity. Then, the full-width-at-half-maximum(FWHM) and binding energy of neutral donor bound excition were 7meV and 5.9meV, respectivity. by Haynes rule, an activation energy of impurity was 50 meV.

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Effects of B Doping on Structural, Optical, and Electrical Properties of ZnO Nanorods Grown by Hydrothermal Method

  • Kim, Soaram;Nam, Giwoong;Park, Hyunggil;Yoon, Hyunsik;Kim, Byunggu;Kim, Jin Soo;Kim, Jong Su;Leem, Jae-Young
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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    • pp.337-337
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    • 2013
  • ZnO seed layers were deposited on a quartz substrate using the sol-gel method, and B-doped ZnO (BZO) nanorods with different B concentrations ranging from 0 to 2.5 at.% were grown on the ZnO seed layers by the hydrothermal method. The structural, optical, electrical propertiesof the ZnO and BZO nanorods were investigated using field-emission scanning electron microscopy, X-ray diffraction (XRD), photoluminescence (PL), ultraviolet-visible spectroscopy, and hall effect. The ZnO and BZO nanorods grew well aligned on the surface of the quartz substrates. From the XRD data, it can be seen that the B doping is responsible for the distortion of the ZnO lattice. The PL spectra show near-band-edge emission and deep-level emission, and they also show that B doping significantly affects the PL properties of ZnO nanorods. The optical band gaps are changed by B doping, and thus the Urbach energy value changed with the optical band gap of the ZnO nanorods. From the hall measurements, it can be observed that the values of electrical resistivity, carrier concentration, and mobility are changed by B doping.

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Hot Wall Epitaxy (W)에 의한 ZnIn$_2$S$_4$ 단결정 박막 성장과 특성 (Growth and characterization of ZnIn$_2$S$_4$ single crystal thin film using Hot Wall Epitaxy method)

  • 윤석진;홍광준
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2002년도 하계학술대회 논문집
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    • pp.266-272
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    • 2002
  • The stochiometric mixture of evaporating materials for the ZnIn$_2$S$_4$ single crystal thin film was prepared from horizontal furnace. To obtain the ZnIn$_2$S$_4$ single crystal thin film, ZnIn$_2$S$_4$ mixed crystal was deposited on throughly etched semi-insulating GaAs(100) in the Hot Wall Epitaxy(HWE) system. The source and substrate temperature were 610 $^{\circ}C$ and 450 $^{\circ}C$, respectively and the growth rate of the ZnIn$_2$S$_4$ single crystal thin film was about 0.5 $\mu\textrm{m}$/hr. The crystalline structure of ZnIn$_2$S$_4$ single crystal thin film was investigated by photo1uminescence and double crystal X-ray diffraction(DCXD) measurement. The carrier density and mobility of ZnIn$_2$S$_4$ single crystal thin film measured from Hall effect by van der Pauw method are 8.51${\times}$10$\^$17/ cm$\^$-3/, 291 $\textrm{cm}^2$/V$.$s at 293 $^{\circ}$K, respectively. From the photocurrent spectrum by illumination of perpendicular light on the c - axis of the ZnIn$_2$S$_4$ single crystal thin film, we have found that the values of spin orbit splitting ΔSo and the crystal field splitting ΔCr were 0.0148 eV and 0.1678 eV at 10 $^{\circ}$K, respectively. From the photoluminescence measurement of ZnIn$_2$S$_4$ single crystal thin film, we observed free excition (E$\_$X/) typically observed only in high quality crystal and neutral donor bound exciton (D$^{\circ}$,X) having very strong peak intensity. The full width at half maximum and binding energy of neutral donor bound excition were 9 meV and 26 meV, respectively. The activation energy of impurity measured by Haynes rule was 130 meV.

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$AgGaSe_2$ 단결정 박막 성장과 광전기적 특성 (Growth and Optoelectrical Properties for $AgGaSe_2$ Single Crystal Thin Films)

  • 홍광준;유상하
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2004년도 추계학술대회 논문집 Vol.17
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    • pp.171-174
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    • 2004
  • The stochiometric $AgGaSe_2$ polycrystalline mixture of evaporating materials for the $AgGaSe_2$ single crystal thin film was prepared from horizontal furnace. To obtain the single crystal thin films, $AgGaSe_2$ mixed crystal and semi-insulating GaAs(100) wafer were used as source material and substrate for the Hot Wall Epitaxy (HWE) system, respectively. The source and substrate temperature were fixed at $630^{\circ}C$ and $420^{\circ}C$, respectively. The thickness of grown single crystal thin films is $2.1{\mu}m$. The single crystal thin films were investigated by photoluminescence and double crystal X-ray diffraction(DCXD) measurement. The carrier density and mobility of $AgGaSe_2$ single crystal thin films measured from Hall effect by van der Pauw method are $4.89{\times}10^{17}\;cm^{-3},\;129cm^2/V{\cdot}s$ at 293K, respectively. From the photocurrent spectrum by illumination of perpendicular light on the c - axis of the $AgGaSe_2$ single crystal thin film, we have found that the values of spin orbit splitting ${\Delta}S_o$ and the crystal field splitting ${\Delta}C_r$ were 0.1762 eV and 0.2494 eV at 10 K, respectively. From the photoluminescence measurement of $AgGaSe_2$ single crystal thin film, we observed free excition $(E_X)$ observable only in high quality crystal and neutral bound exciton $(D^o,X)$ having very strong peak intensity And, the full width at half maximum and binding energy of neutral donor bound excition were 8 meV and 14.1 meV, respectively. By Haynes rule, an activation energy of impurity was 141 meV.

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저온 공정 PVP게이트 절연체를 이용한 고성능 플렉서블 유기박막 트랜지스터의 계면처리 효과 (Interface Treatment Effect of High Performance Flexible Organic Thin Film Transistor (OTFT) Using PVP Gate Dielectric in Low Temperature)

  • 윤호진;백규하;신홍식;이가원;이희덕;도이미
    • 한국전기전자재료학회논문지
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    • 제24권1호
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    • pp.12-16
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    • 2011
  • In this study, we fabricated the flexible pentacene TFTs with the polymer gate dielectric and contact printing method by using the silver nano particle ink as a source/drain material on plastic substrate. In this experiment, to lower the cross-linking temperature of the PVP gate dielectric, UV-Ozone treatment has been used and the process temperature is lowered to $90^{\circ}C$ and the surface is optimized by various treatment to improve device characteristics. We tried various surface treatments; $O_2$ Plasma, hexamethyl-disilazane (HMDS) and octadecyltrichlorosilane (OTS) treatment methods of gate dielectric/semiconductor interface, which reduces trap states such as -OH group and grain boundary in order to improve the OTFTs properties. The optimized OTFT shows the device performance with field effect mobility, on/off current ratio, and the sub-threshold slope were extracted as $0.63cm^2 V^{-1}s^{-1}$, $1.7{\times}10^{-6}$, and of 0.75 V/decade, respectively.

Staggered and Inverted Staggered Type Organic-Inorganic Hybrid TFTs with ZnO Channel Layer Deposited by Atomic Layer Deposition

  • Gong, Su-Cheol;Ryu, Sang-Ouk;Bang, Seok-Hwan;Jung, Woo-Ho;Jeon, Hyeong-Tag;Kim, Hyun-Chul;Choi, Young-Jun;Park, Hyung-Ho;Chang, Ho-Jung
    • 마이크로전자및패키징학회지
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    • 제16권4호
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    • pp.17-22
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    • 2009
  • Two different organic-inorganic hybrid thin film transistors (OITFTs) with the structures of glass/ITO/ZnO/PMMA/Al (staggered structure) and glass/ITO/PMMA/ZnO/Al (inverted staggered structure), were fabricated and their electrical and structural properties were compared. The ZnO thin films used as active channel layers were deposited by the atomic layer deposition (ALD) method at a temperature of $100^{\circ}C$. To investigate the effect of the substrates on their properties, the ZnO films were deposited on bare glass, PMMA/glass and ITO/glass substrates and their crystal properties and surface morphologies were analyzed. The structural properties of the ZnO films varied with the substrate conditions. The ZnO film deposited on the ITO/glass substrate showed better crystallinity and morphologies, such as a higher preferred c-axis orientation, lower FWHM value and larger particle size compared with the one deposited on the PMMA/glass substrate. The field effect mobility ($\mu$), threshold voltage ($V_T$) and $I_{on/off}$ switching ratio for the OITFT with the staggered structure were about $0.61\;cm^2/V{\cdot}s$, 5.5 V and $10^2$, whereas those of the OITFT with the inverted staggered structure were found to be $0.31\;cm^2/V{\cdot}s$, 6.8 V and 10, respectively. The improved electrical properties for the staggered OITFTs may originate from the improved crystal properties and larger particle size of the ZnO active layer.

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