倒置通道mosfet在硅上的3C-SiC

J. Wan, M. Capano, M. Melloch, J. Cooper
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引用次数: 5

摘要

摘要:作为衬底材料,单晶SiC晶圆的直径可达75 mm,而硅晶圆的直径可达75 mm。直径为200-300毫米。与硅相比,碳化硅晶圆仍然相当昂贵,并且含有令人烦恼的微管密度,这限制了大型设备的产量。在过去,一些研究小组试图通过在硅衬底上外延生长的3C-SiC薄膜中制造器件来规避这些问题,但收效甚微。然而,在本文中,我们报告了在硅上的3C-SiC薄膜中展示高质量反转沟道mosfet的新结果。由于带隙上半部分的高密度界面态,SiC mosfet的反转通道迁移率在4H多型中被限制在< 50 cm2JVs,在6H多型中被限制在< 100 cm2fVs。由于其更窄的带隙,3C多型SiC有望具有更低的界面态密度,从而导致更高的通道迁移率。我们在6引脚的p型层中制备了横向n沟道mosfet,该层生长在20个离轴Si(001)衬底上。随后抛光脱毛层以提高表面光滑度,留下3%的厚度层。然后进行牺牲氧化以去除抛光造成的损伤。在1250℃氩气中活化30分钟,注入磷形成源、排。在1150℃下湿氧化30分钟形成栅极氧化物,然后在950℃的湿O2中再氧化2小时。采用LPCVD沉积多晶硅栅极,并掺杂自旋掺杂剂。欧姆触点是未退火的镍。所得到的mosfet表现出优异的晶体管性能,具有良好的电流饱和度,1.6 V的阈值电压和170 cm2/Vs的峰值通道迁移率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Inversion channel MOSFETs in 3C-SiC on silicon
Abstract : As a substrate material, single crystal SiC wafers are commercially available in diameters up to 75 mm, whereas silicon wafers a?e available in diameters of 200-300 mm. SiC wafers remain quite expensive compared to silicon, and contain%troublesome densities of micropipes that limit the yield of large devices. In the past, several groups have attempted to circumvent these problems by fabricating devices in 3C-SiC films grown epitaxially on silicon substrates, with limited success. However, in this paper we report new results demonstrating high quality inversion channel MOSFETs in 3C-SiC films on silicon. The inversion channel mobility of SiC MOSFETs has been limited to < 50 cm2JVs in the 4H polytype and < 100 cm2fVs in the 6H polytype by a high density of interface states in the upper half of the bandgap. Because of its narrower bandgap, the 3C polytype of SiC is expected to have lower interface state density, leading to higher channel mobilities. We fabricated lateral n-channel MOSFETs in 6 pin p-type epilayers of 3C-SiC grown on 20 off-axis Si(001) substrates. The epilayers were subsequently polished to improve surface smoothness, leaving a 3 %im layer. Sacrificial oxidation was then performed to remove damage caused by polishing. Source and drains were formed by implanting phosphorus and activating at 1250 0C for 30 minutes in argon. The gate oxide was formed by wet oxidation at 1150 0C for 30 minutes, followed by re-oxidation in wet O2 at 950 0C for two hours. A polysilicon gate was deposited by LPCVD and doped by spin-on dopant. Ohmic contacts are unannealed nickel. The resulting MOSFETs show excellent transistor behavior, with good current saturation, a threshold voltage of 1.6 V, and a peak channel mobility of 170 cm2/Vs.
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