999精品在线视频,手机成人午夜在线视频,久久不卡国产精品无码,中日无码在线观看,成人av手机在线观看,日韩精品亚洲一区中文字幕,亚洲av无码人妻,四虎国产在线观看 ?

Testing and Characterization of GaN-based MOSFET at Space Cryogenic Temperature

2021-12-15 14:35:42XIAOYipingWANGYaningLIUChaomingZHANGYanqingQIChunhuaWANGTianqiMAGuoliangHUOMingxueLUYudongYUELong
原子能科學(xué)技術(shù) 2021年12期

XIAO Yiping, WANG Yaning, LIU Chaoming,*, ZHANG Yanqing, QI Chunhua, WANG Tianqi, MA Guoliang, HUO Mingxue, LU Yudong, YUE Long

(1.Space Environment Simulation Research Infrastructure, Harbin Institute of Technology, Harbin 150001, China; 2.Guangzhou GRG Metrology & Test Co., Ltd., Guangzhou 510000, China)

Abstract: Deep space exploration applications require electronics which are capable of operation at extremely low temperatures (T<40 K). Based on the application requirements of cryogenic temperatures, the effects of cryogenic temperatures from 15 K to 300 K on GaN-based MOSFET were investigated in this paper. The experimental results show that the saturated drain current and threshold voltage are increased as the device is cooled down to 15 K. Both output characteristics and transfer characteristics are enhanced as temperature decreases. The increase of electron migration rate could be the main reason for the shift of electrical parameters of GaN-based MOSFET.

Key words:GaN; MOSFET; cryogenic temperature; characterization

1 Introduction

GaN, as a typical third-generation semiconductor material, is widely used in increasingly harsh conditions due to wide band gap, high saturation drift speed, good thermal stability and high critical breakdown electric field[1-2]. GaN-based MOSFET not only solves the defect of the traditional GaN HEMT, but also has remarkable temperature characteristics[3], which has been closely noticed by researchers and become the focus of experimental research. For MgO/GaN MOSFET, analysis of the output characteristics and breakdown characteristics from 20 ℃ to 500 ℃ on the device shows that break-down voltage and saturation drain current are hardly reduced within 20-500 ℃[4]. Besides, significant decrease of gate drain at elevated temperature was observed on Pt/Ga2O3/GaN MOSFET relative to a conventional Pt/GaN MOSFET, and MOSFET device operation in fact improved upon heating to 400 ℃. Modeling of the high temperature effect on contact resistance shows that the improvement can be attributed to a reduction in the parasitic resistances present in the device[5]. The influence of temperature on the transient switching rate of GaN-based MOSFET was also studied. AtRG=100 Ω, dVGS/dtincreases as the device is cooled from 100 ℃ to -20 ℃, and the temperature characteristics of GaN devices decrease with the decline of migration rate, which contributes to lower wastage and better transient performance[6].

In space, electronic systems that performing tasks in deep space and icy celestial bodies will be subject to ultra-low temperature environment[7-8]. Operation in the most interesting extra-terrestrial locations requires a spacecraft to be capable of surviving any number of harsh conditions. More efficient and reliable performance of the device functioning at the harsh condition is fully needed[9-11]. However, previous work evaluating GaN-based MOSFET device response has focused primarily on high temperature field, so the study of this device at cryogenic temperatures is indispensable.

In this paper, the GaN-based MOSFET is cooled from 15 K to 300 K by a low temperature test platform. The goal of this research has been not only the assessment of the performance of GaN-based MOSFET for cryogenic operations but also the achievement of a better understanding of the physical mechanism involved with temperature-induced effects in active devices. The response of these devices to extreme environments will contribute to the design and manufacture of GaN-based MOSFET in space applications and demonstrate the viability of their use in future systems.

2 Device under test and experimental setups

N-channel GaN-based MOSFET used in this paper was produced by Ganpower (Foshan) Co., Ltd. The size of the device is 3923 μm×1222 μm, doped material is mainly PAD, top metal layer is AlCu, which contains a very small amount of Cu. The thickness of substrate Si is 280 μm and GaN layer is 20 μm, respectively.

In order to satisfy the requirements of the cryogenic experiment, the liquid helium-free optical window cryostat produced by JANIS was used. This cryogenic system concludes a Sumitomo CH-204N two-stage cold head, with an HC-4A air-cooled compressor, and cools by compressing and expanding helium. About 10-6Pa vacuum and about 15 K low temperatures can be provided without consuming liquid helium or liquid nitrogen. A dual independent channel temperature controller (Cryo.con 22C) was used to monitor and control the temperature of the cold head and the DUT. Temperature readings were taken with a T-type thermocouple mounted in the cold head and a Si diode (Lake Shore DT-670, 1.4-500 K) near the DUT. Pins of the tested sample are connected with the electrical connector so as to realize the test of the electrical performance parameters of the sample. The experimental test set-up is shown in Fig.1.

Fig.1 Experimental test set-up

TheI-Vmeasurements including output characteristics and transfer characteristics were carried out by using Keithley 2636B source meter. The device was slowly cooled from 300 K to 15 K over a period of time. As the device cooled, the parameter analyzer sweep was run at 20 K intervals, producing a complete set ofI-Vcurves at each temperature point.

3 Results and analyses

Temperature plays an important role on the electrical and physical characteristics of semiconductor materials. When transistors are exposed to extremely cold temperatures, their operation is altered in the semiconductor material characteristics. The positive outputIDS-VDScurves of GaN-based MOSFET from 15 K to 300 K atVGS=4 V are shown in Fig.2. It can be seen that the drain currentIDSis increased at a given drain voltage, while the drain voltageVDSis degraded at the same drain current with the decreasing temperature. AtVDS=0-5 V, drain currentIDSincreases as enhancedVDS, thenIDSbasically maintains a stable value and positive output curve reaches a saturated state withVDSincreases to more than 5 V.

Fig.2 Positive output curves IDS-VDS of GaN-based MOSFET for several temperatures at VGS=4 V

Fig.3 Saturation drain current IDSS of GaN-based MOSFET under different temperatures

The saturated drain currents of GaN-based MOSFET for several different temperatures are shown in Fig.3. There is a sharp rising trend ofIDSSnear the room temperature and the rate of increase inIDSSgradually levels off as the temperature drops below 160 K. The plot can be explained in the following manner. Starting at room temperature, the initial increase in current is on account of a reduction in the electron-phonon scattering rate. However, the increase of impurity scattering rate begins cancel out the electron-phonon scattering effect at lower temperatures[12]. Finally, the electronic migration rate maintains an equilibrium state andIDSSincreases steadily.

RDS_ONof GaN-based MOSFET under different temperatures is shown in Fig.4. Based on previous studies,RDS_ONis defined the ratio of drain voltage to drain current at the unsaturated zone of output curve,RDS_ON=VDS/IDS. It can be seen that the on-state resistanceRDS_ONdecreases over the entire range of the temperature points. The on-state resistanceRDS_ONdecreases by about 6.8% as the device is cooled from 280 K to 15 K, and reaches a minimum value ofRDS_ON=10.48 Ω at 15 K. The lower on-state resistance contributes to the higher drain current, the lower wastage and the better operating characteristics.

Fig.4 On-state resistances of GaN-based MOSFET at VGS=4 V under different temperatures

The current versus temperature curves in the saturation (VDS=8 V,VGS=4 V) and linear triode (VDS=5 V,VGS=4 V) regions of operation are shown in Fig.5. It is apparent that current in the linear region has very similar temperature dependence to that in the saturation region, indicating that dIDS/dTchanges slightly and self-heating effects barely appear under the experiment.

The trend ofIDS-VGSof the GaN-based MOSFET transfer characteristic curve in the range of 15-300 K is shown in Fig.6. The current shows a similar increase at lower temperature as in the previous output characteristics curve. WhenVGSincrease from 0 to 1 V, the drain currentIDSgrows very slowly, at this time the conversion characteristics are not sensitive to temperature changes, however whenVGSincreases from 1 V to 2 V, theIDSincreases rapidly withVGS, and the rate increases faster when the temperature is lower. Such improvements inIDS-VGScharacteristics with decreasing temperature are consistent with previous work on Si bulk FinFETs[12-13].

Fig.5 Linear triode and saturation regions of GaN-based MOSFET under different temperatures

Fig.6 Transfer curves of IDS-VGS of GaN-based MOSFET for several temperatures

Threshold voltageVthfor several temperatures is shown in Fig.7. Significant increase in threshold voltage with temperature decrease is typical for GaN-based MOSFET and has been observed in both implanted DMOSFETs. This temperature dependence is explained by the high density of acceptor-like states near the conduction band edge. At relatively high temperatures, the possibility of negative charge of electrons captured by interface trap drops, the negative charge on interface decreases, and the threshold voltage decreases accordingly[14-15]. As a result, increased threshold voltage proves higher switching rate.

Fig.7 Threshold voltages of GaN-based MOSFET under different temperatures

From the analysis of Fig.6 and Fig.7, it can be found that the cryogenic temperature environment can also improve the transfer characteristics of GaN-based MOSFET devices to some extent.

4 Conclusion

In summary, the electrical performance of GaN-based MOSFET at temperatures from 15 K to 300 K is demonstrated and analyzed. It is found that with a decrease of operation temperature, the threshold voltage and saturated drain current increase monotonously, while the on-state resistance drops. The shift of threshold voltage of GaN-based MOSFET at cryogenic temperature is due to high interface state trappings. And the increase of saturated drain current contributes to high electronic mobility.

GaN-based MOSFET continues to function properly as temperature decrease to 15 K both on output and transfer performances and shows excellent enhanced cryogenic characteristics under the conditions of this study, indicating that GaN-based MOSFET can be capable of surviving low temperatures as cooled as 15 K.

主站蜘蛛池模板: 久久99国产综合精品1| 伊人色综合久久天天| 国产成人av一区二区三区| 国产成人精品三级| 欧美日韩亚洲综合在线观看| 日本人真淫视频一区二区三区| 精品福利国产| 日韩欧美中文| 欧美视频免费一区二区三区| 无码视频国产精品一区二区| 71pao成人国产永久免费视频| 国产成人精品一区二区三区| 凹凸国产熟女精品视频| 欧美亚洲激情| 久久国产乱子| 1024你懂的国产精品| 亚洲制服丝袜第一页| 久夜色精品国产噜噜| 国产h视频免费观看| 国内黄色精品| 国产一区二区色淫影院| 激情视频综合网| 国产综合亚洲欧洲区精品无码| 国产情侣一区| 亚洲男人天堂网址| 蜜芽国产尤物av尤物在线看| 亚洲国产系列| 国产成人综合网在线观看| 亚洲视频在线观看免费视频| 日韩av手机在线| 国内精品九九久久久精品| 日韩毛片基地| 亚洲啪啪网| 亚洲欧美在线综合一区二区三区 | 亚洲最新在线| 亚洲bt欧美bt精品| 国产原创自拍不卡第一页| 国产成人无码AV在线播放动漫| 性网站在线观看| 99re精彩视频| 亚洲一区二区约美女探花| 久久精品国产电影| 精品国产91爱| 亚洲Aⅴ无码专区在线观看q| 亚洲高清中文字幕| 亚洲人成网站色7799在线播放| 色综合成人| 国内精自视频品线一二区| 免费人成视频在线观看网站| 99精品在线视频观看| 制服丝袜 91视频| 第九色区aⅴ天堂久久香| 国产视频大全| 亚洲中文字幕无码mv| 久久国产V一级毛多内射| 免费在线成人网| 黑色丝袜高跟国产在线91| 亚洲无码A视频在线| 免费福利视频网站| 国产成人8x视频一区二区| 午夜视频免费试看| 亚洲国产精品日韩专区AV| 国产精品女人呻吟在线观看| 91av国产在线| 热99re99首页精品亚洲五月天| 国产超薄肉色丝袜网站| 爆操波多野结衣| 伊人久久精品无码麻豆精品 | 国产美女人喷水在线观看| 国产成在线观看免费视频| 性色在线视频精品| 亚洲天堂首页| 日韩国产一区二区三区无码| 又黄又爽视频好爽视频| 亚洲综合色婷婷| 国产又粗又猛又爽视频| 日韩在线影院| 女人18毛片一级毛片在线| 91无码人妻精品一区二区蜜桃| 乱人伦视频中文字幕在线| 秋霞国产在线| 国产幂在线无码精品|