• Title/Summary/Keyword: breakdown potential

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The Analysis of Breakdown Voltage for the Double-gate MOSFET Using the Gaussian Doping Distribution

  • Jung, Hak-Kee
    • Journal of information and communication convergence engineering
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    • v.10 no.2
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    • pp.200-204
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    • 2012
  • This study has presented the analysis of breakdown voltage for a double-gate metal-oxide semiconductor field-effect transistor (MOSFET) based on the doping distribution of the Gaussian function. The double-gate MOSFET is a next generation transistor that shrinks the short channel effects of the nano-scaled CMOSFET. The degradation of breakdown voltage is a highly important short channel effect with threshold voltage roll-off and an increase in subthreshold swings. The analytical potential distribution derived from Poisson's equation and the Fulop's avalanche breakdown condition have been used to calculate the breakdown voltage of a double-gate MOSFET for the shape of the Gaussian doping distribution. This analytical potential model is in good agreement with the numerical model. Using this model, the breakdown voltage has been analyzed for channel length and doping concentration with parameters such as projected range and standard projected deviation of Gaussian function. As a result, since the breakdown voltage is greatly changed for the shape of the Gaussian function, the channel doping distribution of a double-gate MOSFET has to be carefully designed.

Simulation on Surface Tracking Pattern using the Dielectric Breakdown Model

  • Kim, Jun-Won;Roh, Young-Su
    • Journal of Electrical Engineering and Technology
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    • v.6 no.3
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    • pp.391-396
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    • 2011
  • The tracking pattern formed on the dielectric surface due to a surface electrical discharge exhibits fractal structure. In order to quantitatively investigate the fractal characteristics of the surface tracking pattern, the dielectric breakdown model has been employed to numerically generate the surface tracking pattern. In dielectric breakdown model, the pattern growth is determined stochastically by a probability function depending on the local electric potential difference. For the computation of the electric potential for all points of the lattice, a two-dimensional discrete Laplace equation is solved by mean of the successive over-relaxation method combined to the Gauss-Seidel method. The box counting method has been used to calculate the fractal dimensions of the simulated patterns with various exponent $\eta$ and breakdown voltage $\phi_b$. As a result of the simulation, it is found that the fractal nature of the surface tracking pattern depends strongly on $\eta$ and $\phi_b$.

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.

Analysis of Breakdown Voltages of Double Gate MOSFET Using 2D Potential Model (이차원 전위분포모델을 이용한 이중게이트 MOSFET의 항복전압 분석)

  • Jung, Hakkee
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.17 no.5
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    • pp.1196-1202
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    • 2013
  • This paper have analyzed the change of breakdown voltage for channel doping concentration and device parameters of double gate(DG) MOSFET using two dimensional potential model. The low breakdown voltage becomes the obstacle of power device operation, and breakdown voltage decreases seriously by the short channel effects derived from scaled down device in the case of DGMOSFET. The two dimensional analytical potential distribution derived from Poisson's equation have been used to analyze the breakdown voltage for device parameters such as channel length, channel thickness, gate oxide thickness and channel doping concentration. Resultly, we could observe the breakdown voltage has greatly influenced on device dimensional parameters as well as channel doping concentration, especially the shape of Gaussian function used as channel doping concentration.

Electrical Breakdown Characteristics of LN2 under Simulated Quenching Conditions for Application of HTS Apparatus (고온초전도 기기응용을 위한 모의 \ulcorner치 환경에서 액체질소의 절연파괴 특성)

  • 백승명;정종만;김상현
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.15 no.11
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    • pp.985-990
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    • 2002
  • The electrical breakdown characteristics of liquid nitrogen(LN$\sub$2/) were studied under simulated quenching conditions for application of HTS apparatus. The experimental results for various quenching condition revealed that the breakdown voltage of LN$\sub$2/ with bubble flow velocity and gap spacing. In the case, breakdown voltage decreases gradually with the bubble velocity. When it is bubble velocity from 0 to 1 $\ell$ /min, breakdown voltage rapidly decreases but decreases from 2 $\ell$/min to 10 $\ell$/min slowly. The breakdown voltage for vertical electrode arrangement is higher than that for horizontal electrode arrangement. Also, it did a electric field and potential distribution interpreting at the liquid nitrogen when the bubble existed. The plots of equipotential lines for three cases are also shown.

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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A Study on the Breakdown Characteristics of High Voltage Device using Field Limiting Ring and Side Glass Insulator Wall (전계제한테와 측면 유리 절연층을 사용한 고내압 소자의 항복 특성 연구)

  • Huh, Chang-Su;Chu, Eun-Sang
    • Proceedings of the KIEE Conference
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    • 1995.07c
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    • pp.1072-1074
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    • 1995
  • Zinc-Borosilicate is used as a side insulastor wall to make high breakdown voltage with one Field Limiting Ring in a p-n junction. It is known that surface charge can be yield at the interface of Zinc-Borosilicate Glass/Silicon system. When the glass is used as a side insulator wall, surface charge varied potential distribution and breakdown voltage improved more than 660V without using more FLR.

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Relation between Conduction Path and Breakdown Voltages of Double Gate MOSFET (DGMOSFET의 전도중심과 항복전압의 관계)

  • Jung, Hakkee
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.17 no.4
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    • pp.917-921
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    • 2013
  • This paper have analyzed the change of breakdown voltage for conduction path of double gate(DG) MOSFET. The low breakdown voltage among the short channel effects of DGMOSFET have become obstacles of device operation. The analytical solution of Poisson's equation have been used to analyze the breakdown voltage, and Gaussian function been used as carrier distribution to analyze closely for experimental results. The change of breakdown voltages for conduction path have been analyzed for device parameters such as channel length, channel thickness, gate oxide thickness and doping concentration. Since this potential model has been verified in the previous papers, we have used this model to analyze the breakdown voltage. Resultly, we know the breakdown voltage is greatly influenced on the change of conduction path for device parameters of DGMOSFET.

Diamond Schottky Barrier Diodes With Field Plate (필드 플레이트가 설계된 다이아몬드 쇼트키 장벽 다이오드)

  • Chang, Hae Nyung;Kang, Dong-Won;Ha, Min-Woo
    • The Transactions of The Korean Institute of Electrical Engineers
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    • v.66 no.4
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    • pp.659-665
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    • 2017
  • Power semiconductor devices required the low on-resistance and high breakdown voltage. Wide band-gap materials opened a new technology of the power devices which promised a thin drift layer at an identical breakdown voltage. The diamond had the wide band-gap of 5.5 eV which induced the low power loss, high breakdown capability, low intrinsic carrier generation, and high operation temperature. We investigated the p-type pseudo-vertical diamond Schottky barrier diodes using a numerical simulation. The impact ionization rate was material to calculating the breakdown voltage. We revised the impact ionization rate of the diamond for adjusting the parallel-plane breakdown field at 10 MV/cm. Effects of the field plate on the breakdown voltage was also analyzed. A conventional diamond Schottky barrier diode without field plate exhibited the high forward current of 0.52 A/mm and low on-resistance of $1.71{\Omega}-mm$ at the forward voltage of 2 V. The simulated breakdown field of the conventional device was 13.3 MV/cm. The breakdown voltage of the conventional device and proposed devices with the $SiO_2$ passivation layer, anode field plate (AFP), and cathode field plate (CFP) was 680, 810, 810, and 1020 V, respectively. The AFP cannot alleviate the concentration of the electric field at the cathode edge. The CFP increased the breakdown voltage with evidences of the electric field and potential. However, we should consider the dielectric breakdown because the ideal breakdown field of the diamond is higher than that of the $SiO_2$, which is widely used as the passivation layer. The real breakdown voltage of the device with CFP decreased from 1020 to 565 V due to the dielectric breakdown.

Breakdown voltage improvement of LDMOS using Trench Gate structure (Trench Gate 구조를 이용한 LDMOS의 항복전압 개선)

  • Kim, Hyoung-Woo;Yoo, Seung-Jin;Chung, Sang-Koo
    • Proceedings of the KIEE Conference
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    • 1999.07d
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    • pp.1938-1940
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    • 1999
  • Trench-Gate structures are proposed to improve the breakdown voltage of LDMOS as well as the second breakdown under forward biased gate. Two dimensional device simulator PISCES II has been used to explain the effects of the drift layer thickness on the breakdown voltage of the conventional LDMOS and Trench Gate LDMOS in terms of potential contour lines. The Trench Gate structure has shown improvements in the breakdown voltage by about 44% and 84% for $V_G$=0 V and $V_G$=15 V respectively.

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