实现具有优异直流和射频性能的热可靠增强型InAlAs/InGaAs/InP hemt的工艺开发

Weifeng Zhao, Niu Jin, Guang Chen, Vipan Kumar, I. Adesida
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Using FATFETs and C-V measurements, it was demonstrated that no gate diffusion occurred in thermally-treated Ir-gate E-HEMTs whereas there was gate diffusion in Pt-gate devices [4]. In this work, we have combined the Ir-gate contact and Ge/Ag/Ni-ohmic contact technologies to fabricate high performance E-HEMTs with high thermal stability potential. The heterostructure used for this study was grown by molecular beam epitaxy on (100) semi-insulating InP substrate. The schematic is shown in Fig. 1. The sheet resistance, sheet carrier concentration, and electron mobility, as determined by Hall measurements, were 253 Q/z, 2.97 x 1012 cm-2 and 8295 cm2/V-S, respectively. Ohmic contact optimization process based on transmission line method (TLM) with metallization of Ge/Ag/Ni was first performed to determine the optimum annealing conditions for ohmic formation. Also, Schottky diodes using Ir/Ti/Pt/Au contact metallization were fabricated to study Schottky barrier height enhancement as a function of annealing temperature. Both the TLM samples and Schottky diodes were passivated using a 60-nm-thick SiNX layer prior to annealing in a rapid thermal annealing (RTA) system for 30 seconds. Device fabrication starts with mesa and sidewall isolations using a mixture of citric acid and hydrogen peroxide. The metallization of Ge/Ag/Ni was then deposited using electron beam evaporation and lift-off techniques for ohmic contact. T-shaped gate was defined by e-beam lithography system. The following recess procedure was performed after the gate definition: the 8-nm-thick Ino.53Ga047As contact layer and 6-nm-thick undoped In0o52A10o48As layer was first selectively removed using a citric acid/hydrogen peroxide solution. Then the first AlAs etch stop layer was removed by a solution of HCl and DI water in the ratio of 1: 2. Using the same solution of citric acid, the 3.5-nm-thick undoped Ino52A1048As D-HEMT barrier layer was subsequently removed followed by the removal of the second layer of AlAs etch stop by the same HCl solution that was used for the first AlAs layer. After the gate recess, Ir/Ti/Pt/Au were evaporated by e-beam evaporator. Before the ohmic and gate contacts were annealed simultaneously, a SiNX layer was deposited by PECVD. This SiNx layer also acted as the passivation layer for the final device. The sample was annealed at 425 °C for 30 seconds in a rapid thermal annealing (RTA) system. After annealing, an overlay metal stack of Ti/Pt/Au was deposited. The gate width and source-drain spacing of the devices were 100 ptm and 2 ptm, respectively Figure 2 shows a minimum contact resistance of 0.1 Q-mm at an annealing temperature of 425 'C. Figure 3 shows that Schottky diodes based on Ir/Ti/Pt/Au metallization on nW-InAlAs yielded the highest barrier height at 824 meV when it was annealed at 400 'C. At an annealing temperature of 425 'C, the barrier height was 820 meV. Figure 4 shows the forward current and ideality factor of the Schottky diode that was thermally-treated at 425 'C. Based on these results, a simultaneous thermal treatment for the Schottky gate and ohmic contact at 425 'C for 30 sec was adopted for device fabrication. E-HEMTs with gate-lengths of 0.1 ptm and 0.25 ptm were fabricated. Excellent DC and RF characteristics for the 0.1 ptm gate-length device are shown in Figs. 5 and 6, with VT of 198 mV, Gm,max of 945 mS/mm, ID,maxof 435 mA/mm (drain current at VG = 0.7 V, VD = 1.OV), IDSS of 0.25 mA/mm (drain current at VG= 0 V, VD= 1.0 V), andfT of 205 GHz. The threshold voltage andfT for the device with a gate-length of 0.25 ptm were 259 mV and 86 GHz, respectively. In conclusion, we have developed a novel fabrication process for E-HEMTs based on Ir-gate and Ge/Ag/Niohmic contact technologies. In addition to excellent DC and RF performances, these E-HEMTs are expected to be highly thermally stable. Results on thermal stability will be presented. These metallization have also been applied to depletion-mode with excellent results. References [1] J. A. Del Alamo et al.. IEDM Tech. Dig, pp. 44.1.1, Dec. 2004. [2] M. Dammann et al,AMicroelectronics Reliability, 44, pp. 939, 2004 [3] W. Zhao et at., Electron Dev. Lett. 27, pp.4, 2006 [4] S. 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They are annealed at temperatures higher than those used for conventionally annealed-AuGe/Ni/Au ohmic contacts. Schottky contacts based on Iridium have been shown to have barrier heights as high as Platinum-based Schottky contacts [4]. E-HEMTs fabricated utilizing Ir-gate have demonstrated better thermal stability than Pt-gate E-HEMTs [4]. Using FATFETs and C-V measurements, it was demonstrated that no gate diffusion occurred in thermally-treated Ir-gate E-HEMTs whereas there was gate diffusion in Pt-gate devices [4]. In this work, we have combined the Ir-gate contact and Ge/Ag/Ni-ohmic contact technologies to fabricate high performance E-HEMTs with high thermal stability potential. The heterostructure used for this study was grown by molecular beam epitaxy on (100) semi-insulating InP substrate. The schematic is shown in Fig. 1. The sheet resistance, sheet carrier concentration, and electron mobility, as determined by Hall measurements, were 253 Q/z, 2.97 x 1012 cm-2 and 8295 cm2/V-S, respectively. Ohmic contact optimization process based on transmission line method (TLM) with metallization of Ge/Ag/Ni was first performed to determine the optimum annealing conditions for ohmic formation. Also, Schottky diodes using Ir/Ti/Pt/Au contact metallization were fabricated to study Schottky barrier height enhancement as a function of annealing temperature. Both the TLM samples and Schottky diodes were passivated using a 60-nm-thick SiNX layer prior to annealing in a rapid thermal annealing (RTA) system for 30 seconds. Device fabrication starts with mesa and sidewall isolations using a mixture of citric acid and hydrogen peroxide. The metallization of Ge/Ag/Ni was then deposited using electron beam evaporation and lift-off techniques for ohmic contact. T-shaped gate was defined by e-beam lithography system. The following recess procedure was performed after the gate definition: the 8-nm-thick Ino.53Ga047As contact layer and 6-nm-thick undoped In0o52A10o48As layer was first selectively removed using a citric acid/hydrogen peroxide solution. Then the first AlAs etch stop layer was removed by a solution of HCl and DI water in the ratio of 1: 2. Using the same solution of citric acid, the 3.5-nm-thick undoped Ino52A1048As D-HEMT barrier layer was subsequently removed followed by the removal of the second layer of AlAs etch stop by the same HCl solution that was used for the first AlAs layer. After the gate recess, Ir/Ti/Pt/Au were evaporated by e-beam evaporator. Before the ohmic and gate contacts were annealed simultaneously, a SiNX layer was deposited by PECVD. This SiNx layer also acted as the passivation layer for the final device. The sample was annealed at 425 °C for 30 seconds in a rapid thermal annealing (RTA) system. After annealing, an overlay metal stack of Ti/Pt/Au was deposited. The gate width and source-drain spacing of the devices were 100 ptm and 2 ptm, respectively Figure 2 shows a minimum contact resistance of 0.1 Q-mm at an annealing temperature of 425 'C. Figure 3 shows that Schottky diodes based on Ir/Ti/Pt/Au metallization on nW-InAlAs yielded the highest barrier height at 824 meV when it was annealed at 400 'C. At an annealing temperature of 425 'C, the barrier height was 820 meV. Figure 4 shows the forward current and ideality factor of the Schottky diode that was thermally-treated at 425 'C. Based on these results, a simultaneous thermal treatment for the Schottky gate and ohmic contact at 425 'C for 30 sec was adopted for device fabrication. E-HEMTs with gate-lengths of 0.1 ptm and 0.25 ptm were fabricated. 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引用次数: 1

摘要

欧姆接触退化和栅极下沉(特别是当Pt用作e - hemt的栅极接触时)是InAlAs/InGaAs/InP hemt的两个主要可靠性问题[1,2]。基于Ge/Ag/Ni金属化的热稳定欧姆触点最近得到了发展。它们在比传统退火的auge /Ni/Au欧姆触点更高的温度下退火。基于铱的肖特基触点已被证明具有与基于铂的肖特基触点[4]一样高的障壁高度。利用ir栅极制备的E-HEMTs比pt栅极制备的E-HEMTs具有更好的热稳定性。使用fatfet和C-V测量,证明在热处理的ir栅极e - hemt中没有栅极扩散,而在pt栅极器件[4]中有栅极扩散。在这项工作中,我们结合了Ir-gate接触和Ge/Ag/ ni -欧姆接触技术来制造具有高热稳定电位的高性能e - hemt。本研究采用分子束外延法在(100)半绝缘InP衬底上生长异质结构。原理图如图1所示。通过霍尔测量,薄片电阻、载流子浓度和电子迁移率分别为253 Q/z、2.97 x 1012 cm-2和8295 cm2/V-S。首先进行了Ge/Ag/Ni金属化的传输线法(TLM)欧姆接触优化工艺,确定了欧姆形成的最佳退火条件。此外,利用Ir/Ti/Pt/Au接触金属化制备了肖特基二极管,研究了退火温度对肖特基势垒高度增强的影响。在快速热退火(RTA)系统中退火30秒之前,TLM样品和肖特基二极管都使用60 nm厚的SiNX层进行钝化。设备制造从台面和侧壁隔离开始,使用柠檬酸和过氧化氢的混合物。然后利用电子束蒸发和欧姆接触升空技术沉积了Ge/Ag/Ni的金属化。采用电子束光刻系统定义t形栅极。在栅极定义后,进行以下隐层操作:首先使用柠檬酸/过氧化氢溶液选择性去除8nm厚的no. 53ga047as接触层和6nm厚的未掺杂in052a1048as层。然后用盐酸和去离子水按1:2的比例溶液去除第一层AlAs蚀刻停止层。随后使用相同的柠檬酸溶液去除3.5 nm厚的未掺杂的Ino52A1048As D-HEMT势垒层,然后使用用于第一层AlAs的相同的HCl溶液去除第二层AlAs蚀刻停止。栅极凹槽后,用电子束蒸发器蒸发Ir/Ti/Pt/Au。在欧姆触点和栅极触点同时退火之前,用PECVD沉积了一层SiNX层。这个SiNx层也作为最终器件的钝化层。样品在425°C快速热退火(RTA)系统中退火30秒。退火后,沉积了Ti/Pt/Au金属叠加层。器件的栅极宽度和源漏间距分别为100 ptm和2 ptm,图2显示了在425℃退火温度下的最小接触电阻为0.1 Q-mm。图3显示了基于nW-InAlAs上Ir/Ti/Pt/Au金属化的肖特基二极管在400℃退火时产生的最高势垒高度为824 meV,退火温度为425℃时,势垒高度为820 meV。图4显示了在425℃下进行热处理的肖特基二极管的正向电流和理想因数。基于这些结果,采用在425℃下对肖特基栅极和欧姆接触同时热处理30秒的方法进行器件制造。制备栅极长度分别为0.1 ptm和0.25 ptm的e- hemt。图5和图6显示了0.1 ptm门长器件优异的直流和射频特性,其VT为198 mV, Gm,max为945 mS/mm, ID,max为435 mA/mm(漏极电流为VG= 0.7 V, VD= 1 V), IDSS为0.25 mA/mm(漏极电流为VG= 0 V, VD= 1.0 V), ft为205 GHz。对于门长为0.25 ptm的器件,阈值电压和ft分别为259 mV和86 GHz。总之,我们开发了一种基于Ir-gate和Ge/Ag/ niomic接触技术的新型e - hemt制造工艺。除了优异的直流和射频性能外,这些e - hemt还有望具有高度的热稳定性。将给出热稳定性的结果。这些金属化也已应用于耗尽模式,并取得了良好的效果。参考文献b[1] J. A. Del Alamo等。IEDM technology . Dig, pp. 44.1.1, december 2004。[10]赵伟等,微电子技术与可靠性,2004,第4期,第939页。,电子开发学报,27,pp.4, 2006, bbb10 .金等,DRC Dig。,第259页,2005。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Process development for the realization of thermally-reliable enhancement-mode InAlAs/InGaAs/InP HEMTs with excellent DC and RF performance
Ohmic contact degradation and gate sinking (especially when Pt is used as the gate contact for E-HEMTs) are two of the major reliability concerns for the InAlAs/InGaAs/InP HEMTs [1, 2]. Thermally-stable Ohmic contacts based on Ge/Ag/Ni metallizations have recently been developed [3]. They are annealed at temperatures higher than those used for conventionally annealed-AuGe/Ni/Au ohmic contacts. Schottky contacts based on Iridium have been shown to have barrier heights as high as Platinum-based Schottky contacts [4]. E-HEMTs fabricated utilizing Ir-gate have demonstrated better thermal stability than Pt-gate E-HEMTs [4]. Using FATFETs and C-V measurements, it was demonstrated that no gate diffusion occurred in thermally-treated Ir-gate E-HEMTs whereas there was gate diffusion in Pt-gate devices [4]. In this work, we have combined the Ir-gate contact and Ge/Ag/Ni-ohmic contact technologies to fabricate high performance E-HEMTs with high thermal stability potential. The heterostructure used for this study was grown by molecular beam epitaxy on (100) semi-insulating InP substrate. The schematic is shown in Fig. 1. The sheet resistance, sheet carrier concentration, and electron mobility, as determined by Hall measurements, were 253 Q/z, 2.97 x 1012 cm-2 and 8295 cm2/V-S, respectively. Ohmic contact optimization process based on transmission line method (TLM) with metallization of Ge/Ag/Ni was first performed to determine the optimum annealing conditions for ohmic formation. Also, Schottky diodes using Ir/Ti/Pt/Au contact metallization were fabricated to study Schottky barrier height enhancement as a function of annealing temperature. Both the TLM samples and Schottky diodes were passivated using a 60-nm-thick SiNX layer prior to annealing in a rapid thermal annealing (RTA) system for 30 seconds. Device fabrication starts with mesa and sidewall isolations using a mixture of citric acid and hydrogen peroxide. The metallization of Ge/Ag/Ni was then deposited using electron beam evaporation and lift-off techniques for ohmic contact. T-shaped gate was defined by e-beam lithography system. The following recess procedure was performed after the gate definition: the 8-nm-thick Ino.53Ga047As contact layer and 6-nm-thick undoped In0o52A10o48As layer was first selectively removed using a citric acid/hydrogen peroxide solution. Then the first AlAs etch stop layer was removed by a solution of HCl and DI water in the ratio of 1: 2. Using the same solution of citric acid, the 3.5-nm-thick undoped Ino52A1048As D-HEMT barrier layer was subsequently removed followed by the removal of the second layer of AlAs etch stop by the same HCl solution that was used for the first AlAs layer. After the gate recess, Ir/Ti/Pt/Au were evaporated by e-beam evaporator. Before the ohmic and gate contacts were annealed simultaneously, a SiNX layer was deposited by PECVD. This SiNx layer also acted as the passivation layer for the final device. The sample was annealed at 425 °C for 30 seconds in a rapid thermal annealing (RTA) system. After annealing, an overlay metal stack of Ti/Pt/Au was deposited. The gate width and source-drain spacing of the devices were 100 ptm and 2 ptm, respectively Figure 2 shows a minimum contact resistance of 0.1 Q-mm at an annealing temperature of 425 'C. Figure 3 shows that Schottky diodes based on Ir/Ti/Pt/Au metallization on nW-InAlAs yielded the highest barrier height at 824 meV when it was annealed at 400 'C. At an annealing temperature of 425 'C, the barrier height was 820 meV. Figure 4 shows the forward current and ideality factor of the Schottky diode that was thermally-treated at 425 'C. Based on these results, a simultaneous thermal treatment for the Schottky gate and ohmic contact at 425 'C for 30 sec was adopted for device fabrication. E-HEMTs with gate-lengths of 0.1 ptm and 0.25 ptm were fabricated. Excellent DC and RF characteristics for the 0.1 ptm gate-length device are shown in Figs. 5 and 6, with VT of 198 mV, Gm,max of 945 mS/mm, ID,maxof 435 mA/mm (drain current at VG = 0.7 V, VD = 1.OV), IDSS of 0.25 mA/mm (drain current at VG= 0 V, VD= 1.0 V), andfT of 205 GHz. The threshold voltage andfT for the device with a gate-length of 0.25 ptm were 259 mV and 86 GHz, respectively. In conclusion, we have developed a novel fabrication process for E-HEMTs based on Ir-gate and Ge/Ag/Niohmic contact technologies. In addition to excellent DC and RF performances, these E-HEMTs are expected to be highly thermally stable. Results on thermal stability will be presented. These metallization have also been applied to depletion-mode with excellent results. References [1] J. A. Del Alamo et al.. IEDM Tech. Dig, pp. 44.1.1, Dec. 2004. [2] M. Dammann et al,AMicroelectronics Reliability, 44, pp. 939, 2004 [3] W. Zhao et at., Electron Dev. Lett. 27, pp.4, 2006 [4] S. Kim et al., DRC Dig., pp. 259, 2005.
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