Performance Improvement by SiO₂ Hardmask in 100-nm InP-Based HEMTs for TMIC Applications

Benzocyclobutene (BCB) has been widely used as passivation and interlayer dielectric for sub-millimeter-wave applications and terahertz monolithic microwave integrated circuits (TMICs). In this work, the influence of BCB passivation on 100-nm InP-based high-electron-mobility transistors (HEMTs) was investigated. A set of 100-nm HEMTs with different gate recess structures were fabricated and compared. A SiO2 hard mask was adopted in the gate recess, which contributed to an improved device performance after BCB passivation. DC and RF performances were characterized before and after BCB passivation. The results show that BCB passivation in the recess region degraded InP HEMTs’ performance, and a better performance was achieved by the SiO2 hard mask. For traditional devices, of which the gate recess was exposed to silicon nitride (SiNx) and BCB passivation layers, both dc and RF performances were deteriorated drastically even though the thickness of SiNx passivation layer was increased from 20 to 50 nm. However, the SiO2 hard mask preserved the device performances to a great degree, with only degradation by increased parasitic capacitances according to the small-signal equivalent model. In addition, the threshold voltage shift after BCB passivation was suppressed by the SiO2 hard mask. Thus, a device structure suitable for BCB passivated TMIC applications is proposed and validated.

[1]  X. Wallart,et al.  75 nm Gate Length PHEMT With fmax = 800 GHz Using Asymmetric Gate Recess: RF and Noise Investigation , 2021, IEEE Transactions on Electron Devices.

[2]  Daehyun Kim,et al.  Lg = 19 nm In0.8Ga0.2As composite-channel HEMTs with fT = 738 GHz and fmax = 492 GHz , 2020, 2020 IEEE International Electron Devices Meeting (IEDM).

[3]  Zhi Jin,et al.  Surface Improvement of InAlAs/InGaAs InP-Based HEMT Through Treatments of UV/Ozone and TMAH , 2020, IEEE Journal of the Electron Devices Society.

[4]  Daehyun Kim,et al.  ${L}_{{g}} = {87}$ nm InAlAs/InGaAs High-Electron- Mobility Transistors With a g m_max of 3 S/mm and $f , 2018, IEEE Electron Device Letters.

[5]  William R. Deal,et al.  850 GHz Receiver and Transmitter Front-Ends Using InP HEMT , 2017, IEEE Transactions on Terahertz Science and Technology.

[6]  C. Chen,et al.  Ultra-thin 20 nm-PECVD-Si 3 N 4 surface passivation in T-shaped gate InAlAs/InGaAs InP-based HEMTs and its impact on DC and RF performance , 2016 .

[7]  A. Leuther,et al.  Submillimeter-Wave Amplifier Circuits Based on Thin Film Microstrip Line Front-Side Technology , 2015, 2015 IEEE Compound Semiconductor Integrated Circuit Symposium (CSICS).

[8]  W. Deal,et al.  First Demonstration of Amplification at 1 THz Using 25-nm InP High Electron Mobility Transistor Process , 2015, IEEE Electron Device Letters.

[9]  W. R. Deal,et al.  InP HEMT for sub-millimeter wave space applications: Status and challenges , 2014, 2014 39th International Conference on Infrared, Millimeter, and Terahertz waves (IRMMW-THz).

[10]  W. Deal,et al.  Recent progress in scaling InP HEMT TMIC technology to 850 GHz , 2014, 2014 IEEE MTT-S International Microwave Symposium (IMS2014).

[11]  W. Deal,et al.  Low Noise Amplification at 0.67 THz Using 30 nm InP HEMTs , 2011, IEEE Microwave and Wireless Components Letters.

[12]  Daehyun Kim,et al.  30-nm InAs Pseudomorphic HEMTs on an InP Substrate With a Current-Gain Cutoff Frequency of 628 GHz , 2008, IEEE Electron Device Letters.

[13]  Hong Wang,et al.  Investigation of drain current transient in BCB-and SiN-passivated Al0.25Ga0.75As/In0- 2Ga0- 8As pseudomorphic high electron mobility transistors , 2007 .

[14]  Hsien-Chin Chiu,et al.  High performance BCB-bridged AlGaAs/InGaAs power HFETs , 2003 .

[15]  D. Schreurs,et al.  Influence of silicon nitride passivation on DC and RF behaviour of InP HEMTs , 2002, The 10th IEEE International Symposium on Electron Devices for Microwave and Optoelectronic Applications.

[16]  Yasuhiro Nakasha,et al.  Enhancement of $f_{\mathrm {max}}$ to 910 GHz by Adopting Asymmetric Gate Recess and Double-Side-Doped Structure in 75-nm-Gate InAlAs/InGaAs HEMTs , 2017, IEEE Transactions on Electron Devices.

[17]  B. Brar F T = 688 Ghz and F Max = 800 Ghz in L G = 40 Nm in 0.7 Ga 0.3 as Mhemts with G M_max > 2.7 Ms/μm , 2011 .