• Title/Summary/Keyword: Gate charge

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The recess gate structure for the improvement of breakdown characteristics of GaAs MESFET (GaAs MESFET의 파괴특성 향상을 위한 recess게이트 구조)

  • 장윤영;송정근
    • Electrical & Electronic Materials
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    • v.7 no.5
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    • pp.376-382
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    • 1994
  • In this study we developed a program(DEVSIM) to simulate the two dimensional distribution of the electrostatic potential and the electric field of the arbitrary structure consisting of GaAs/AlGaAs semiconductor and metal as well as dielectric. By the comparision of the electric field distribution of GaAs MESFETs with the various recess gates we proposed a suitable device structure to improve the breakdown characteristics of MESFET. According to the results of simulation the breakdown characteristics were improved as the thickness of the active epitaxial layer was decreased. And the planar structure, which had the highly doped layer under the drain for the ohmic contact, was the worst because the highly doped layer prevented the space charge layer below the gate from extending to the drain, which produced the narrow spaced distribution of the electrostatic potential contours resulting in the high electric field near the drain end. Instead of the planar structure with the highly doped drain the recess gate structure having the highly doped epitaxial drain layer show the better breakdown characteristics by allowing the extention of the space charge layer to the drain. Especially, the structure in which the part of the drain epitaxial layer near the gate show the more improvement of the breakdown characteristics.

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Potential Barrier Shift Caused by Channel Charge in Short Channel GaAs MESFET (Short Channel GaAs MESFET의 채널전하분포와 채널전하에 의한 전위장벽의 변화)

  • Sub, Won-Chang;Lee, Myung-Soo;Ryu, Se-Hwan;Han, Deuk-Young;Ahn, Hyung-Keun
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.19 no.9
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    • pp.793-799
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    • 2006
  • In this paper, the gate leakage current is first calculated using the experimental method between gate and drain by opening source electrode. the gate to drain current has been obtained with ground source. The difference between two currents has been tested and proves that the electric field generated by channel charge effect against the image force lowering.

Investigation of Junction-less Tunneling Field Effect Transistor (JL-TFET) with Floating Gate

  • Ali, Asif;Seo, Dongsun;Cho, Il Hwan
    • JSTS:Journal of Semiconductor Technology and Science
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    • v.17 no.1
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    • pp.156-161
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    • 2017
  • This work presents a novel structure for junction-less tunneling field effect transistor (JL-TFET) with a floating gate over the source region. Introduction of floating gate instead of fixed metal gate removes the limitation of fabrication process suitability. The proposed device is based on a heavily n-type-doped Si-channel junction-less field effect transistor (JLFET). A floating gate over source region and a control-gate with optimized metal work-function over channel region is used to make device work like a tunnel field effect transistor (TFET). The proposed device has exhibited excellent ID-VGS characteristics, ION/IOFF ratio, a point subthreshold slope (SS), and average SS for optimized device parameters. Electron charge stored in floating gate, isolation oxide layer and body doping concentration are optimized. The proposed JL-TFET can be a promising candidate for switching performances.

Electrical Properties of MOS Capacitors and Transistors with in-situ doped Amorphous Si Gate (증착시 도핑된 비정질 Si 게이트를 갖는 MOS 캐패시터와 트랜지스터의 전기적 특성)

  • 이상돈;이현창;김재성;김봉렬
    • Journal of the Korean Institute of Telematics and Electronics A
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    • v.31A no.6
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    • pp.107-116
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    • 1994
  • In this paper, The electrical properties of MOS capacitors and transistoras with gate of in-situ doped amorphous Si and poly Si doped by POCI$_3$. Under constant current F-N stress, MOS capacitors with in-situ doped amorphous Si gate have shown the best resistance to degradation in reliabilty properties such as increase of leakage current, shift of gate voltage (V$_{g}$). shift of flat band voltage (V$_{fb}$) and charge to breakdown(Q$_{bd}$). Also, MOSFETs with in-situ doped amorphous Si gate have shown to have less degradation in transistor properties such as threshold voltage, transconductance and drain current. These improvements observed in MOS devices with in-situ doped amorphous Si gate is attributed to less local thinning spots at the gate/SiO$_2$ interface, caused by the large grain size and the smoothness of the surface at the gate/SiO$_2$ interface.

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A VPP Generator Design for a Low Voltage DRAM (저전압 DRAM용 VPP Generator 설계)

  • Kim, Tae-Hoon;Lee, Jae-Hyung;Ha, Pan-Bong;Kim, Young-Hee
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2007.10a
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    • pp.776-780
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    • 2007
  • In this paper, the charge pump circuit of a VPP generator for a low voltage DRAM is newly proposed. The proposed charge pump is a 2-stage cross coupled charge pump circuit. The charge transfer efficiency is improved, and Distributed Clock Inverter is located in each charge pump stage to reduce clock period so that the pumping current is increased. In addition, the precharge circuit is located at Gate node of charge transfer transistor to solve the problem which is that the Gate node is maintained high voltage because the boosted charge can't discharge, so device reliability is decreased. The simulation result is that pumping current, pumping efficiency and power efficiency is improved. The layout of the proposed VPP generator is designed using $0.18{\mu}m$ Triple-Well process.

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Dickson Charge Pump with Gate Drive Enhancement and Area Saving

  • Lin, Hesheng;Chan, Wing Chun;Lee, Wai Kwong;Chen, Zhirong;Zhang, Min
    • Journal of Power Electronics
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    • v.16 no.3
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    • pp.1209-1217
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    • 2016
  • This paper presents a novel charge pump scheme that combines the advantages of Fibonacci and Dickson charge pumps to obtain 30 V voltage for display driver integrated circuit application. This design only requires four external capacitors, which is suitable for a small-package application, such as smart card displays. High-amplitude (<6.6 V) clocks are produced to enhance the gate drive of a Dickson charge pump and improve the system's current drivability by using a voltage-doubler charge pump with a pulse skip regulator. This regulation engages many middle-voltage devices, and approximately 30% of chip size is saved. Further optimization of flying capacitors tends to decrease the total chip size by 2.1%. A precise and simple model for a one-stage Fibonacci charge pump with current load is also proposed for further efficiency optimization. In a practical design, its voltage error is within 0.12% for 1 mA of current load, and it maintains a 2.83% error even for 10 mA of current load. This charge pump is fabricated through a 0.11 μm 1.5 V/6 V/32 V process, and two regulators, namely, a pulse skip one and a linear one, are operated to maintain the output of the charge pump at 30 V. The performances of the two regulators in terms of ripple, efficiency, line regulation, and load regulation are investigated.

Breakdown Characteristics of Silicon Nanowire N-channel GAA MOSFET (실리콘 나노와이어 N-채널 GAA MOSFET의 항복특성)

  • Ryu, In Sang;Kim, Bo Mi;Lee, Ye Lin;Park, Jong Tae
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.20 no.9
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    • pp.1771-1777
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    • 2016
  • In this thesis, the breakdown voltage characteristics of silicon nanowire N-channel GAA MOSFETs were analyzed through experiments and 3-dimensional device simulation. GAA MOSFETs with the gate length of 250nm, the gate dielectrics thickness of 6nm and the channel width ranged from 400nm to 3.2um were used. The breakdown voltage was decreased with increasing gate voltage but it was increased at high gate voltage. The decrease of breakdown voltage with increasing channel width is believed due to the increased current gain of parasitic transistor, which was resulted from the increased potential in channel center through floating body effects. When the positive charge was trapped into the gate dielectrics after gate stress, the breakdown voltage was decreased due to the increased potential in channel center. When the negative charge was trapped into the gate dielectrics after gate stress, the breakdown voltage was increased due to the decreased potential in channel center. We confirmed that the measurement results were agreed with the device simulation results.

Electrical characteristics of SiC thin film charge trap memory with barrier engineered tunnel layer

  • Han, Dong-Seok;Lee, Dong-Uk;Lee, Hyo-Jun;Kim, Eun-Kyu;You, Hee-Wook;Cho, Won-Ju
    • Proceedings of the Korean Vacuum Society Conference
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    • 2010.08a
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    • pp.255-255
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    • 2010
  • Recently, nonvolatile memories (NVM) of various types have been researched to improve the electrical performance such as program/erase voltages, speed and retention times. Also, the charge trap memory is a strong candidate to realize the ultra dense 20-nm scale NVM. Furthermore, the high charge efficiency and the thermal stability of SiC nanocrystals NVM with single $SiO_2$ tunnel barrier have been reported. [1-2] In this study, the SiC charge trap NVM was fabricated and electrical properties were characterized. The 100-nm thick Poly-Si layer was deposited to confined source/drain region by using low-pressure chemical vapor deposition (LP-CVD). After etching and lithography process for fabricate the gate region, the $Si_3N_4/SiO_2/Si_3N_4$ (NON) and $SiO_2/Si_3N_4/SiO_2$ (ONO) barrier engineered tunnel layer were deposited by using LP-CVD. The equivalent oxide thickness of NON and ONO tunnel layer are 5.2 nm and 5.6 nm, respectively. By using ultra-high vacuum magnetron sputtering with base pressure 3x10-10 Torr, the 2-nm SiC and 20-nm $SiO_2$ were successively deposited on ONO and NON tunnel layers. Finally, after deposited 200-nm thick Al layer, the source, drain and gate areas were defined by using reactive-ion etching and photolithography. The lengths of squire gate are $2\;{\mu}m$, $5\;{\mu}m$ and $10\;{\mu}m$. The electrical properties of devices were measured by using a HP 4156A precision semiconductor parameter analyzer, E4980A LCR capacitor meter and an Agilent 81104A pulse pattern generator system. The electrical characteristics such as the memory effect, program/erase speeds, operation voltages, and retention time of SiC charge trap memory device with barrier engineered tunnel layer will be discussed.

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A New DC-DC Converter for Gate Driver Circuit Using Low Temperature Poly-Si TFT

  • Choi, Jin-Young;Cho, Byoung-Chul;Shim, Hyun-Sook;Kwon, Oh-Kyong
    • 한국정보디스플레이학회:학술대회논문집
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    • 2004.08a
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    • pp.1011-1014
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    • 2004
  • In this paper, we present a new DC-DC converter for gate driver circuit in low temperature poly-Si TFT technology. It is composed of a newly developed charge pump circuit and a regulator circuit. When the input voltage is 5V, the efficiency of a positive charge pump used in the DC-DC converter and that of a negative charge pump is 69.0% and 57.1%, respectively. The output voltage of DC-DC converter varies 200mV when the target voltages of DC-DC converter are 9V, -6V and the threshold voltage of TFTs varies ${\pm}$ 0.5V.

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Low-Temperature Poly-Si TFT Charge Trap Flash Memory with Sputtered ONO and Schottky Junctions

  • An, Ho-Myoung;Kim, Jooyeon
    • Transactions on Electrical and Electronic Materials
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    • v.16 no.4
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    • pp.187-189
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    • 2015
  • A charge-trap flash (CTF) thin film transistor (TFT) memory is proposed at a low-temperature process (≤ 450℃). The memory cell consists of a sputtered oxide-nitride-oxide (ONO) gate dielectric and Schottky barrier (SB) source/drain (S/D) junctions using nickel silicide. These components enable the ultra-low-temperature process to be successfully achieved with the ONO gate stacks that have a substrate temperature of room temperature and S/D junctions that have an annealing temperature of 200℃. The silicidation process was optimized by measuring the electrical characteristics of the Ni-silicided Schottky diodes. As a result, the Ion/Ioff current ratio is about 1.4×105 and the subthreshold swing and field effect mobility are 0.42 V/dec and 14 cm2/V·s at a drain voltage of −1 V, respectively.