A Compact D-Band Phase Shifter with 0.1-degree Phase Resolution and 0.8-degree RMS Phase Error in 65 nm CMOS
Sub-THz phased-array transceivers play an important role in future 6th-generation mobile communication systems (6G). In particular, the phase shifter is an essential circuit for phased-array transceivers. The phase shifter must have high-resolution phase steps and low phase error to achieve high-precision beam steering and calibration [1]. This work presents a high-precision D-band cascaded phase shifter for 6 G wireless communications. The active fine-tuning phase shifter with feedback technology realizes high-resolution phase shifting. This technology achieves over three times the fine phase shift of conventional works with lower power consumption. In addition, a compact propagation delay phase shifter using a non-uniform architecture is proposed. Thanks to this technique, a 360-degree phase shift with low phase error and reduced insertion loss is realized. The proposed phase shifter achieves a phase step of 0.1° and RMS phase error of 0.8° within the frequency range of 150-160 GHz. The power consumption is 5 mW, and the IC core area is $0.099 \mathrm{~mm}^{2}$, fabricated in a 65 nm CMOS process.
Authors
- Hiroyuki Sakai (ORCID: https://orcid.org/0000-0001-7144-1549)
- Sungwan Park
- Chenxin Liu (ORCID: https://orcid.org/0000-0002-5645-3688)
- Atsushi Shirane (ORCID: https://orcid.org/0000-0001-8172-4323)
- Yudai Yamazaki (ORCID: https://orcid.org/0000-0001-9061-541X)
- Kazuaki Kunihiro (ORCID: https://orcid.org/0000-0003-1163-4976)
- A. Bahgat Shehata (ORCID: https://orcid.org/0000-0002-9258-3367)
- Kenichi Okada (ORCID: https://orcid.org/0000-0002-1082-7672)
- T. Uchino (ORCID: https://orcid.org/0000-0001-6412-7658)
- Anyi Tian
Institutions
- Tokyo Institute of Technology (JP)
Publication Details
- Published
- 2024-11-18
- DOI
- https://doi.org/10.1109/a-sscc60305.2024.10848583
- Citations
- 2
- Primary Topic
- Radio Frequency Integrated Circuit Design
- Type
- article
- Field-Weighted Citation Impact
- 0.42