GaInAsAnP composite channel HEMTs

M. Matioubian, L.M. Jellolan, M. Lul, T. Liu, L. Larson, L. Nguyen, M. Le
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引用次数: 2

Abstract

GalnAs/AllnAs on InP HEMTs have demonstrated great potential for microwave and millimeter wave power applications [1,2]. By using Al,lnl-,As Schottky layer with x>0.48 we have been able to improve the gate-to-drain breakdown voltage of these HEMTs. But the remaining drawback has been their low value of the drain-to-source breakdown voltage due to the low breakdown field of the Ga0.47ln0.53As channel. Using InP as the channel material should improve the drain-to-source breakdown voltage, but due to the difficulty in achieving very low contact resis?ances-as well as the higher fields necessary to achieve velocity saturation-InP channel HEMTs have a higher knee voltage in their current-voltage characteristics and lower fT's than typical Gao.47lno.53As channel HEMTs. By using a combination of a thin layer of GalnAs and InP as the channel material it is theoretically possible to use the advantages of both materials [3]. Previously reported composite channel structures did not demonstrate any improvement in the drain-to-source breakdown voltage, probably due to the limitation of the gate-to-drain breakdown voltage of the devices. In this study we have combined AIo.60h0.40As Schottky layers with GalnAsAnP composite channels. We investigated the effect of changing the thickness of the Ga0.471n0.53As channel on the DC and RF characteristics of the HEMTs. The wafers were grown using a Varian Gen I I gas-source MBE on InP substrates. The channel consisted of a 100 A InP layer doped 2X1018cm-3, followed by a 50 A undoped InP layer. The Ga0.47ln0.53As channel thicknesses were varied between the three wafers grown and they were 100 A, 50 A, and 30 A for wafers A, 6, and C respectively. A 250 A Alo.6oino.40As undoped layer was used as the Schottky layer. HEMTs with gate-length of 0.15 pm, drain-to-source spacing of 2 pm, and total gate-widths ranging from 50 to 900 pm were fabricated on these three wafers. Preliminary measured results on the wafers are very encouraging. The maximum transconductance (measured at Vds=l.5 V) for wafers A, 6, and C, were 795, 71 1, and 613 mS/mm. Wafers A, 6, and C, had full channel currents of 733, 747, and 560 mA/mm, and drain-to-source breakdown voltages of 6.8, 8.3, and 10.6 V respectively. The knee voltage on all the wafers were comparable to Ga0.471n0.53As channel HEMTs. Based on the full channel currents and the breakdown voltages, power densities of 480, 627, and 633 mW/mm can be calculated for wafers A, B, and C. The preliminary results indicate that GalnA$/lnP composite channel HEMTs with a Gao.47lno.53As channel thickness of 50 A or less show improvement in the drain-to-source breakdown voltage without sacrificing performance.
GaInAsAnP复合通道hemt
InP hemt上的galna / allna已显示出微波和毫米波功率应用的巨大潜力[1,2]。通过使用x> .48的Al, ln1 -,As肖特基层,我们已经能够提高这些hemt的栅极-漏极击穿电压。但由于Ga0.47ln0.53As通道的击穿场较低,它们的漏源击穿电压值较低。使用InP作为沟道材料可以提高漏源击穿电压,但由于难以实现极低的接触电阻?除了达到速度饱和所需的更高场外,inp沟道hemt在其电流电压特性中具有更高的膝电压,并且比典型的高压电具有更低的fT。53As通道hemt。通过使用galna和InP的薄层组合作为通道材料,理论上可以利用这两种材料的优点。先前报道的复合通道结构在漏极到源极击穿电压方面没有任何改善,可能是由于器件的栅极到漏极击穿电压的限制。在本研究中,我们将AIo.60h0.40As肖特基层与GalnAsAnP复合通道相结合。研究了改变ga0.47 n0.53 as沟道厚度对hemt直流和射频特性的影响。晶圆是使用瓦里安I I型气源MBE在InP衬底上生长的。该通道由一个100a掺杂2X1018cm-3的InP层和一个50a未掺杂的InP层组成。晶圆A、晶圆6和晶圆C的Ga0.47ln0.53As通道厚度分别为100 A、50 A和30 A。a250, a250, a60。40a未掺杂层作为肖特基层。在这三种晶圆上制备了栅极长度为0.15 pm、漏源间距为2 pm、栅极宽度为50 ~ 900 pm的hemt。在硅片上的初步测量结果令人鼓舞。最大跨导(Vds= 1.5)晶圆A、6和C的V)分别为795、71 1和613 mS/mm。晶圆A、6和C的全通道电流分别为733、747和560 mA/mm,漏源击穿电压分别为6.8、8.3和10.6 V。所有晶圆上的膝电压与ga0.47 n0.53 as沟道hemt相当。基于全通道电流和击穿电压,可以计算出A、B、c片的功率密度分别为480mw /mm、627mw /mm和633mw /mm。50a或更小的沟道厚度可以在不牺牲性能的情况下改善漏源击穿电压。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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