• 제목/요약/키워드: N-drift

검색결과 277건 처리시간 0.032초

Effect of Boron Content and Temperature on Interactions and Electron Transport in BGaN Bulk Ternary Nitride Semiconductors

  • Bouchefra, Yasmina;Sari, Nasr-Eddine Chabane
    • Transactions on Electrical and Electronic Materials
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    • 제18권1호
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    • pp.7-12
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    • 2017
  • This work takes place in the context of the development of a transport phenomena simulation based on group III nitrides. Gallium and boron nitrides (GaN and BN) are both materials with interesting physical properties; they have a direct band gap and are relatively large compared to other semiconductors. The main objective of this paper is to study the effect of boron content on the electron transport of the ternary compound $B_xGa_{(1-x)}N$ and the effect of the temperature of this alloy at x=50% boron percentage, specifically the piezoelectric, acoustic, and polar optical scatterings as a function of the energy, and the electron energy and drift velocity versus the applied electric field for different boron compositions ($B_xGa_{(1-x)}N$), at various temperatures for $B_{0.5}Ga_{0.5}N$. Monte carlo simulation, was employed and the three valleys of the conduction band (${\Gamma}$, L, X) were considered to be non-parabolic. We focus on the interactions that do not significantly affect the behavior of the electron. Nevertheless, they are introduced to obtain a quantitative description of the electronic dynamics. We find that the form of the velocity-field characteristic changes substantially when the temperature is increased, and a remarkable effect is observed from the boron content in $B_xGa_{(1-x)}N$ alloy and the applied field on the dynamics of holders within the lattice as a result of interaction mechanisms.

플로팅 아일랜드 구조의 전력 MOSFET의 전기적 특성 분석 (Analysis of The Electrical Characteristics of Power MOSFET with Floating Island)

  • 강이구
    • 한국전기전자재료학회논문지
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    • 제29권4호
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    • pp.199-204
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    • 2016
  • This paper was proposed floating island power MOSFET for lowering on state resistance and the proposed device was maintained 600 V breakdown voltage. The electrical field distribution of floating island power MOSFET was dispersed to floating island between P-base and N-drift. Therefore, we designed higher doping concentration of drift region than doping concentration of planar type power MOSFET. And so we obtain the lower on resistance than on resistance of planar type power MOSFET. We needed the higher doping concentration of floating island than doping concentration of drift region and needed width and depth of floating island for formation of floating island region. We obtained the optimal parameters. The depth of floating island was $32{\mu}m$. The doping concentration of floating island was $5{\times}1,012cm^2$. And the width of floating island was $3{\mu}m$. As a result of designing the floating island power MOSFET, we obtained 723 V breakdown voltage and $0.108{\Omega}cm^2$ on resistance. When we compared to planar power MOSFET, the on resistance was lowered 24.5% than its of planar power MOSFET. The proposed device will be used to electrical vehicle and renewable industry.

Planar Hall Resistance Sensor for Monitoring Current

  • Kim, KunWoo;Torati, Sri Ramulu;Reddy, Venu;Yoon, SeokSoo
    • Journal of Magnetics
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    • 제19권2호
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    • pp.151-154
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    • 2014
  • Recent years have seen an increasing range of planar Hall resistive (PHR) sensor applications in the field of magnetic sensing. This study describes a new application of the PHR sensor to monitor a current. Initially, thermal drift experiments of the PHR sensor are performed, to determine the accuracy of the PHR signal output. The results of the thermal drift experiments show that there is no considerable drift in the signals attained from 0.1, 0.5, 1 and 2 mA current. Consequently, the PHR sensor provides adequate accuracy of the signal output, to perform the current monitoring experiments. The performances of the PHR sensor with bilayer and trilayer structures are then tested. The minimum detectable currents of the PHR sensor using bilayer and trilayer structures are $0.51{\mu}A$ and 54 nA, respectively. Therefore, the PHR sensor having trilayer structure is the better choice to detect ultra low current of few tens nanoampere.

VCO 표류 성분 상쇄기와 빗쌀 하모닉 발생기를 이용한 주파수 대역 확장기의 구현 (Implementation of Frequency Bandwidth Expander using VCO Drift Canceller and Comb generator)

  • 강승민
    • 한국통신학회논문지
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    • 제24권9B호
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    • pp.1683-1689
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    • 1999
  • VCO의 표류성분 제거기와 빗쌀 하모닉 발생기를 이용하여 주파수를 상향 변환하면서 동시에 주파수 대역폭을 확장하는 시스템을 구현하였다. 출력 주파수 범위가 220∼280MHz, 분해능이 5MHz인 저주파수 합성기의 출력을 1660∼2140MHz의 광대역 주파수로 확장한다. 최종출력의 위상 잡음 상태는 저주파수 합성기와 빗쌀 하모닉 발생기에 의해 결정되며 VCO의 표류성분은 최종 출력에 나타나지 않는다. 필터 뱅커처럼 VCO의 조절로 주파수가 60MHz의 단위로 가변되는데 이때의 가변시간은 3usec이하이며, 스퓨리어스는 -55dBc이하이다. VCO의 출력 주파수 범위를 확장하면 쉽게 출력 대역폭을 추가로 확장할 수 있으며, 빠른 스위칭 시간을 요구하는 광대역 초고주파 합성기에 응용될 수 있다.

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한국의 빨간 오징어 유자망 어업과 북서태평양의 해황 변동 (Korean Drift Gillnet Fishery For Flying Squid , Ommastrephes bartrami ( Lesueur ) , and the Variation of Oceanographic Conditions in the North Western Pacific Ocean)

  • 임기봉
    • 수산해양기술연구
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    • 제22권3호
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    • pp.8-16
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    • 1986
  • The fishing conditions of flying squid, ommastrePhes barsram(Lesueur), in the North Pacific Ocean was studied based on the horizontal water temperature data, satellite data from NOAA and statistical data of flying squid fisheries which were collected from 1980 to 1984. The obtained results were as follows; 1. Since 1979, the Korean drift giIlnet fishery for flying squid was launched in North Pacific. Number of operating vessel and catch of flying squid increased gradually every year. The number of vessels were 111 and their annual catches were 42, 977 M/T in 1984. Therefore, Korean drift giIlnet fishery for this species has played an important role in the products of Korean high-sea fisheries. 2. In the beginning of the fisheries, fishing grounds was formed in the west of long. 1800E. In 1982, in consequence of the center which extended eastward, the fishing ground was formed long. 166$^{\circ}$W in the central North Pacific Ocean. Since 1983, the fishing grounds were formed as far as long. 161$^{\circ}$W. The range of general fishing season in the central North Pacific was from June to August. After september, fishing ground was shifted to the west, in the Northwestern Pacific. 3. The Predominant fishing season for the flying squid was August through January of the coming year. Optimum water temperature for flying sguid at surface layer in the Pacific Ocean ranged from 11 $^{\circ}$e to 17$^{\circ}$e in winter, 13$^{\circ}$e to 17$^{\circ}$e in spring, 12. 8$^{\circ}$C to 19.7$^{\circ}$e in summer and 1O.6$^{\circ}$e -18.7$^{\circ}$e in fall. 4. In summer, the Oceanographic condition in the North Pacific Ocean showed that the water temperature at surface layer was lower in 1980, 1983 and higher in 1981, 1982 and 1984 as compared with mean annual water temperature. 5. The characteristics df oceanographic conditions in the fluation, disformation, mixing and other factors of the Kuroshio and Oyashio currents, which have considerably influenced upon the water masses of the areas. 6. The data and information on surface thermal Structure interpreted from Infrared Satellite Imaginary from NOAA-7 and NOAA-8 are very available in estimating water temperature on the areas and investigating the major fishing grounds. 7. According to the fisheries statics of Japanese drift gilInet, the annual catches of flying squid considerably decreased from 225, 942 M/T in 1983 to 133, 217 M/T in 1984. 8. The fishing grounds in the central North Pacific in several fishing seasons were formed as follows: In June, the initial fishing season, the fishing grounds were formed in the vicinity of lat. 35 - 40oN, the central North Pacific east of 179$^{\circ}$E. In July, the fishing ground were formed in the wide arEa of the central North Pacific north of 400N and long. 174$^{\circ}$E-145$^{\circ}$W In Auguest, concentrative fishing operation carried out in :he central North Pacific north of 43$^{\circ}$N and East of 165$^{\circ}$W. On the other hand, in September, main fishing grounds were disappeared and moved to the west.

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$H_2$의 전자 수송 계수에 관한 연구 (A Study on the Electron Transport Coefficients in Hydrogen Molecular)

  • 박은주;전병훈
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2009년도 제40회 하계학술대회
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    • pp.1402_1403
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    • 2009
  • The electron transport coefficients in hydrogen molecular is calculated over the range of E/N values from 0.01 to 300 Td and at temperature state of 77K, 293K and 300K by Boltzmann equation method. The results gained that the values of the electron transport coefficients such as the electron drift velocity, the electron ionization coefficients, longitudinal diffusion coefficients consisted with the results of measured and calculated for a ranage of E/N.

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무전극 램프의 방전가스 연구 (A Study on discharge gas of Fluorescent Induction Lamp)

  • 김근;전병훈
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2009년도 제40회 하계학술대회
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    • pp.1481_1482
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    • 2009
  • Pure Xe, Kr and Ne atoms and Mixures of Xe-Ne used in fluorescent induction lamps(FILs). However standard regulation of FILs is not made up until now. Therefore, the electron transport coefficients, the electron drift velocity W, the longitudinal diffusion coefficient NDL and the ionization coefficient $\alpha$/N in pure Xe, Kr, Ne gases and Xe-Ne mixtures(1:9, 5:5, 7:3) were calculated over the wide E/N range from 0.01 to 500 Td at 1 Torr by two-term approximation of the Boltzman equation.

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서부태평양에서 다랑어 선망어업의 어획분포와 어장환경 (Distribution of Catches and Condition of Fishing Ground for Tuna Purse Seine in the Western Pacific Ocean)

  • 김형석
    • 수산해양기술연구
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    • 제35권3호
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    • pp.227-236
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    • 1999
  • Temperal and spacial analysis for catches have been drawing up a catch distribution chart and analysing catches and CPUE(Catch Per Unit Effort) using catch data with purpose of obtaining basic data to establish a selective method of effective fishing the tuna purse seine fishing ground.The temperature profile section and catch was surveyed to analyse the effect of catch in relation to the fishing ground environment.The results are as follows ;1. As for the catch variation between 1983 and 1984, the catch mainly took place on150^{\circ}E$, and after that it moved eastward enlarging the range of catch. In the monthly catch variation between January and February, the catches mainly happened on 135$^{\circ}$~ 150$^{\circ}$E, and then moved to the gradually westward. However, from July it moved to the South and from October Southeast.2. As to the eatch ratio for the school associated with the drifted object, the pelagic migrating school and the school associated with the biological objects, the catch ratio for the school associated with the drift objects was the highest. The catch ratio for the school associated with the drifted object was high in June, July and November whiles between January and March for the pelagic migrating school.3. SST(Sea Surface Temperature) was around 28~29^C$ on the observing line of 137^{\circ}E$ and the catches took place in the north equatorial counter-current situated on around $5^{\circ}~6^{\circ}N$. SST in the northern summer was 1^C$higher than winter and it was about 29~30^C$. The catch happened with the center of north equatorial counter-current. The reason why the catch mainly took place on the north equatorial counter-current is that main catch of tuna purse seine was the school associated with drift objects. It is thought that the fishing grounds are made in waters that have many drift objects like drift logs from the coast.

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Sol-Gel 법으로 형성한 $Ta_{2}O_{5}$ 게이트 ISFET의 pH 드리프트 특성 (pH-Drift Characteristics of Sol-Gel-Deposited $Ta_{2}O_{5}$-Gate ISFET)

  • 권대혁;조병욱;김창수;손병기
    • 센서학회지
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    • 제5권2호
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    • pp.15-20
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    • 1996
  • 감지막 내부로의 수소이온 확산은 pH-ISFET에서 드리프트로 작용하므로 초박막화된 감지막은 드리프트 시간을 최소화할 것이라는 새로운 인식을 가지고 pH-ISFET의 최대 단점인 드리프트 특성을 개선하기 위하여 sol-gel법으로 $Ta_{2}O_{5}$ 수소이온 감지막을 약 $70{\AA}$정도로 초박막화시킨 ISFET를 제조하고 그 동작특성을 조사하였다. 제조한 $Ta_{2}O_{5}$ 게이트 pH-ISFET는 약 59 mV/pH의 높은 감도를 나타내었고, pH $3{\sim}11$ 범위에서 pH에 따른 ISFET의 출력전압변화는 우수한 선형성을 나타내었으며, 또한 출력전압의 변동에 의한 평균 pH 드리프트는 약 0.06 pH/day로서 비교적 작은 값을 나타내었다.

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