932 resultados para ALGAN SURFACES


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用分子束外延(MBE)技术研制出了AlGaN/GaN高电子迁移率晶体管(HEMT)材料,其室温迁移率为1 035 cm2/Vs、二维电子气浓度为1.0×1013 cm-2;77 K迁移率为2 653 cm2/V*s、二维电子气浓度为9.6×1012 cm-2.用此材料研制了栅长为1 μm、栅宽为80 μm、源-漏间距为4 μm的AlGaN/GaN HEMT,其室温最大非本征跨导为186 mS/mm、最大漏极饱和电流密度为925 mA/mm、特征频率为18.8 GHz.另外,还研制了具有20个栅指(总栅宽为20×80 μm=1.6 mm)的大尺寸器件,该器件的最大漏极饱和电流为1.33 A.

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AlGaN/GaN high electron mobility transistor (HEMT) materials are grown by RF plasma-assisted molecular beam epitaxy (RF-MBE) and HEMT devices are fabricated and characterized. The HEMT materials have a mobility of 1035cm~2/(V ? s) at sheet electron concentration of 1.0 * 10~(13)cm~(-2) at room temperature. For the de-vices fabricated using the malt-rials,a maximum saturation drain-current density of 925mA/mm and a peak extrinsic iransecmductance of IHfimS/mm are obtained on devices with gate length and width of l/-im and 80/im respectively. The f_t, unit-current-gain frequency of the devices,is about 18. 8GHz.

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用自组装的氮源分子束外延(NH_3-MBE)系统和射频等离子体辅助分子束外延(PA-MBE)系统在C面蓝宝石衬底上外延了优质GaN以及AlGaN/GaN二维电子气材料。GaN膜(1.2 μm厚)室温电子迁移率达300 cm~2/V·s,背景电子浓度低至2 * 10~(17) cm~(-3)。双晶X射线衍射(0002)摇摆曲线半高宽为6 arcmin。AlGaN/GaN二维电子气材料最高的室温和77 K二维电子气电子迁移率分别为730 cm~2/V·s和1200 cm~2/V·s,相应的电子面密度分别是7.6 * 10~(12) cm~(-2)和7.1 * 10~(12) cm~(-2);用所外延的AlGaN/GaN二维电子气材料制备出了性能良好的AlGaN/GaN HFET(异质结场效应晶体管),室温跨导为50 mS/mm(栅长1 μm),截止频率达13 GHz(栅长0.5 μm)。该器件在300 ℃出现明显的并联电导,这可能是材料中的深中心在高温被激活所致。

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研究了MOVPE方法外延P型GaN和Al0.13 Ga0.87N的生长工艺,包括掺杂剂量和热退火条件,对材料电学性质的影响。得到了性能优良的P型材料,并研制了InGaN/AlGaN双异质结蓝光发光二极管。

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国家863计划,国家自然科学基金

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于2010-11-23批量导入

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于2010-11-23批量导入

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用射频等离子体辅助分子束外延技术(RF-MBE)在C面蓝宝石衬底上外延了高质量的GaN膜以及AlGaN/GaN极化感应二维电子气材料。所外延的GaN膜室温背景电子浓度为2×10~(17)cm~(-3),相应的电子迁移率为177cm~2/(V·s);GaN(0002)X射线衍射摇摆曲线半高宽(FWHM)为6';AlGaN/GaN极化感应二维电子气材料的室温电子迁移率为730cm~2(V·s),相应的电子气面密度为7.6×10~(12)cm~(-2);用此二维电子气材料制作的异质结场效应晶体管(HFET)室温跨导达50mS/mm(栅长1μm),截止频率达13GHz(栅长0.5μm)。

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报道了用LP-MOVPE技术在蓝宝石(α-Al_2O_3)衬底上生长出以双掺Zn和Si的InGaN为有源区的绿光InGaN/AlGaN双异质结结构,并研制成功发射波长为520-540nm的绿光LED。

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国家863计划,国家自然科学基金

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于2010-11-23批量导入

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Photoluminescence (PL) and temperature-dependent Hall effect measurements were carried out in (0001) and (11 (2) over bar0) AlGaN/GaN heterostructures grown on sapphire substrates by metalorganic chemical vapor deposition. There are strong spontaneous and piezoelectric electric fields (SPF) along the growth orientation of the (0001) AlGaN/GaN heterostructures. At the same time there are no corresponding SPF along that of the (1120) AlGaN/GaN. A strong PL peak related to the recombination between two-dimensional electron gas (2DEG) and photoexcited holes was observed at 3.258 eV at room temperature in (0001) AlGaN/GaN heterointerfaces while no corresponding PL peak was observed in (11 (2) over bar0). The existence of a 2DEG was observed in (0001) AlGaN/GaN multi-layers with a mobility saturated at 6000 cm(2)/V s below 80 K, whereas a much lower mobility was measured in (11 (2) over bar0). These results indicated that the SPF was the main element to cause the high mobility and high sheet-electron-density 2DEG in AlGaN/GaN heterostructures. (C) 2004 Elsevier B.V. All rights reserved.

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Low resistivity of p-type Mg-doped AlGaN/GaN superlattices (SLs) is demonstrated. The resistivity of the SLs is less than 0.6 Omega .cm. and the measured hole concentration is higher than 1x10(18)cm(-3). The resistivity of SLs is much lower, and the hole concentration of SLs is much higher, than that of bulk GaN and AlGaN, The electrical properties of the SLs are less sensitive than the conventional bulk lavers.

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Indium (In)-doping was applied in GaN layers during growth of AlGaN/GaN heterostructure with unintentionally doped or modulation Si-doped AlGaN layers. It was found that In-doping was effective in improving electron sheet density of two-dimensional-electron-gas (2DEG) in the heterostructures. Furthermore, In-doping also improved mobility in heterostructures with Si modulation-doped in AlGaN layers. The possible reasons were discussed. X-ray diffraction (XRD) and wet chemical etching revealed that crystalline quality of GaN was improved by In-doping. It was proposed that In-doping modified growth kinetics of GaN.