单晶金刚石氢终端场效应晶体管特性

基于微波等离子体化学气相淀积生长的单晶金刚石制作了栅长为2μm的耗尽型氢终端金刚石场效应晶体管,并对器件特性进行了分析.器件的饱和漏电流在栅压为-6 V时达到了96 mA/mm,但是在-6 V时栅泄漏电流过大.在-3.5 V的安全工作栅压下,饱和漏电流达到了77 mA/mm.在器件的饱和区,宽5.9 V的栅电压范围内,跨导随着栅电压的增加而近线性增大到30 mS/mm.通过对器件导通电阻和电容-电压特性的分析,氢终端单晶金刚石的二维空穴气浓度达到了1.99×10~(13)cm~(-2),并且迁移率和载流子浓度均随着栅压向正偏方向的移动而逐渐增大.分析认为,沟道中高密度的载流子、大的栅电容以及迁移率的逐渐增加是引起跨导在很大的栅压范围内近线性增加的原因.     

不同晶面的氢终端单晶金刚石场效应晶体管特性

通过微波等离子体化学气相淀积技术生长单晶金刚石并切割得到(110)和(111)晶面金刚石片,以同批器件工艺制备两种晶面上栅长为6μm的氢终端单晶金刚石场效应管,从材料和器件特性两方面对两种晶面金刚石进行对比分析.(110)面和(111)面金刚石的表面形貌在氢终端处理后显著不同,光学性质则彼此相似.VGS=–4 V时,(111)金刚石器件获得的最大饱和电流为80.41 m A/mm,约为(110)金刚石器件的1.4倍;其导通电阻为48.51 W·mm,只有(110)金刚石器件导通电阻的67%.通过对器件电容-电压特性曲线的分析得到,(111)金刚石器件沟道中最大载流子密度与(110)金刚石器件差异不大.分析认为,(111)金刚石器件获得更高饱和电流和更低导通电阻,应归因于较低的方阻.     

氢终端单晶金刚石反相器特性

超宽禁带半导体金刚石材料在高温、高压电路中具有重要的应用潜力.本研究采用微波等离子体化学气相沉积生长的单晶金刚石衬底制备了原子层沉积(atomic layer deposition, ALD)的Al₂O₃栅介质的氢终端金刚石金属氧化物半导体场效应晶体管(metal oxide semiconductor field effect transistor, MOSFET)器件,并与负载电阻互连,成功制备了金刚石反相器. 4μm栅长的氢终端金刚石器件实现了最大113.4 m A/mm的输出饱和漏电流,器件开关比高达109,并在不同负载电阻条件下均成功测得金刚石反相器的电压反转特性,反相器的最大增益为10.     

Semipolar(1122) and polar(0001) InGaN grown on sapphire substrate by using pulsed metal organic chemical vapor deposition

High indium semipolar(1122) and polar(0001) In Ga N layers each with a thickness of about 100 nm are realized simultaneously on sapphire substrates by pulsed metal organic chemical vapor deposition(MOCVD). The morphology evolution, structural and optical characteristics are also studied. The indium content in the layer of the surface(1122)is larger than that of the surface(0001), which is confirmed by reciprocal space map, photoluminescence spectrum and secondary ion mass spectrometer. Additionally, the(0001) surface with island-like morphology shows inhomogeneous indium incorporation, while the(1122) surface with a spiral-like morphology shows a better homogeneous In composition.This feature is also demonstrated by the monochromatic cathodoluminescence map.     

多晶金刚石薄膜硅空位色心形成机理及调控

金刚石硅空位色心在量子信息技术和生物标记领域有重要应用前景.本文对硅衬底上多晶金刚石生长过程中硅空位色心形成机理及调控方法进行研究.通过改变金刚石生长氛围中的氮气和氧气比例,实现了对硅空位色心发光强度的有效调控,所制备系列多晶金刚石样品的光致发光光谱显示,硅空位色心荧光峰与金刚石本征峰的比值最低为1.48,最高可达334.46,该比值与金刚石晶粒尺寸正相关.进一步用光致发光面扫描和拉曼面扫描分析样品可知,多晶金刚石中的硅应来自于硅衬底,在多晶金刚石生长过程中,衬底硅单质先扩散至金刚石晶粒处,随着金刚石晶粒生长,硅单质再扩散并入金刚石晶体结构中形成硅空位色心.不同样品硅空位发光强度的差异,是由于生长过程中氮气和氧气对金刚石硅空位色心的形成分别起到促进和抑制的作用.     

Growth and Characterization of the Laterally Enlarged Single Crystal Diamond Grown by Microwave Plasma Chemical Vapor Deposition

Laterally enlarged single crystal diamond is grown on(001) diamond substrates by microwave plasma chemical vapor deposition. Based on the largest side-to-side width of the seed of 7.5 mm, we achieve the as-grown epilayer with the width of about 10 mm between the same two sides. The luminescence difference between the broadened part of the single crystal diamond and the vertically epitaxial part is investigated by characterizing the vertical cross section of the sample, and the possible growth mechanism is suggested. Vertical epitaxy on the top(001)surface and lateral growth on the side surfaces occur simultaneously, and thus the growth fronts along the two directions adjoin and form a coalescence zone extending from the edge of the substrate towards the edge of the expanded single crystal diamond top surface. The luminescence intensity of the nitrogen-vacancy center is relatively high in the coalescence zone and a laterally grown part right below, which are attributed mainly to the higher growth rate. However, stress change and crystal quality change are negligible near the coalescence zone.     

高跨导氢终端多晶金刚石长沟道场效应晶体管特性研究

基于多晶金刚石制作了栅长为4 pm的铝栅氢终端金刚石场效应晶体管.器件的饱和漏源电流为160 mA/mm,导通电阻低达37.85Ω·mm,最大跨导达到32 mS/mm,且跨导高于最大值的90%的栅压(V_(GS))范围达到3 V(-2 V≤V_(GS)≤-5 V).通过传输线电阻分析以及器件的导通电阻和电容-电压特性分析,发现氢终端多晶金刚石栅下沟道中的空穴面浓度达到了1.56×10~(13)cm~(-2),有效迁移率在前述高跨导栅压范围保持在约170 cm~2/(V·s).分析认为,较低的栅源和栅漏串联电阻、沟道中高密度的载流子和在大范围栅压内的高水平迁移率是引起高而宽阔的跨导峰和低导通电阻的原因.