人工晶体学报
人工晶體學報
인공정체학보
2005年
6期
1006-1010
,共5页
孙国胜%宁瑾%高欣%攻全成%王雷%刘兴昉%曾一平%李晋闽
孫國勝%寧瑾%高訢%攻全成%王雷%劉興昉%曾一平%李晉閩
손국성%저근%고흔%공전성%왕뢰%류흥방%증일평%리진민
4H-SiC%同质外延生长%肖特基二极管
4H-SiC%同質外延生長%肖特基二極管
4H-SiC%동질외연생장%초특기이겁관
4H-SiC%homoepitaxial growth%Schottky barrier diodes
利用台阶控制外延生长技术在偏晶向Si-面衬底上进行了4H-SiC的同质外延生长研究,衬底温度为1500℃,在厚度为32μm、载流子浓度为2~5×1015cm-3的外延材料上制备出了反向阻塞电压大于1kV的Ti/4H-SiC肖特基二极管,二极管的正向与反向电流的整流比(定义偏压为±1V时的电流比值)在室温下超过107,在265℃的温度下超过102,在20~265℃的温度范围内,利用电流电压测量研究了二极管的电学特性,室温下二极管的理想因子和势垒高度分别为1.33和0.905eV,开态电流密度在2.0V的偏压下达到150A/cm2,比开态电阻(Ron)为7.9mΩ·cm2,与温度的关系遵守Ron~T2.0规律.
利用檯階控製外延生長技術在偏晶嚮Si-麵襯底上進行瞭4H-SiC的同質外延生長研究,襯底溫度為1500℃,在厚度為32μm、載流子濃度為2~5×1015cm-3的外延材料上製備齣瞭反嚮阻塞電壓大于1kV的Ti/4H-SiC肖特基二極管,二極管的正嚮與反嚮電流的整流比(定義偏壓為±1V時的電流比值)在室溫下超過107,在265℃的溫度下超過102,在20~265℃的溫度範圍內,利用電流電壓測量研究瞭二極管的電學特性,室溫下二極管的理想因子和勢壘高度分彆為1.33和0.905eV,開態電流密度在2.0V的偏壓下達到150A/cm2,比開態電阻(Ron)為7.9mΩ·cm2,與溫度的關繫遵守Ron~T2.0規律.
이용태계공제외연생장기술재편정향Si-면츤저상진행료4H-SiC적동질외연생장연구,츤저온도위1500℃,재후도위32μm、재류자농도위2~5×1015cm-3적외연재료상제비출료반향조새전압대우1kV적Ti/4H-SiC초특기이겁관,이겁관적정향여반향전류적정류비(정의편압위±1V시적전류비치)재실온하초과107,재265℃적온도하초과102,재20~265℃적온도범위내,이용전류전압측량연구료이겁관적전학특성,실온하이겁관적이상인자화세루고도분별위1.33화0.905eV,개태전류밀도재2.0V적편압하체도150A/cm2,비개태전조(Ron)위7.9mΩ·cm2,여온도적관계준수Ron~T2.0규률.
Homoepitaxial growth of 4H-SiC on off-oriented Si-face (0001) 4H-SiC substrates was performed at 1500℃ by using the step controlled Epitaxy. Ti/4H-SiC Schottky barrier diodes (SBDs) with blocking voltage over 1kV have been made on an undoped epilayer with 32μm in thick and 2-5 × 1015cm-3 in carrier density. The diode rectification ratio of forward to reverse (defined at ± 1 V) is over 107 at room temperature and over 102 at 538K. Their electrical characteristics were studied by the current-voltage measurements in the temperature range from 20 to 265 ℃. The ideality factor and Schottky barrier height obtained at room temperature are 1.33 and 0.905eV, respectively. The SBDs have on-state current density of 150A/cm2 at a forward voltage drop of about 2.0V. The specific on-resistance for the rectifier is found to be as 7.9mΩ·cm2 and its variation with temperature is T2.0.