於此論文中,主要將探討二個針對W頻段通訊系統應用低雜訊放大器之設計、模擬與量測。 在W-band 之無源毫米波(PMMW)頻段,我們提出一個實作在90nm CMOS製程使用 型變壓器和 T 型變壓器技術的94GHz低雜訊法大器(94GHz LNA with and T transformers),藉由使用型變壓器技術雜訊將會被有效地抑制,同時輸入端的阻抗頻寬也會增加。另外 型變壓器技術被使用以便於減少來自閘極電感之串聯電阻的損耗,提昇了此低雜訊放大器的性能。這個低雜訊放大器完成了15.8dB的功率增益、6.8dB的雜訊指數以及適中的35mW功耗。另一個為了防撞雷達及無源毫米波之W 頻段應用的低雜訊放大器(擁有耦合共振腔的W 頻段低雜訊放大器)也被實作在90nm製程。比較先前研究皆以T型匹配網路設計W頻帶低雜訊放大器,本研究提出耦合共振腔之新型匹配網路提供了寬的負載(loading)以便於得到寬的頻寬。另外, 型變壓器技術被採用以便於改善此低雜訊放大器的整體雜訊性能,並且也在輸出端使用T-coil技術去改善輸出端頻寬。這個低雜訊放大器在45mW的功率消耗下完成了11. 87dB的功率增益、7.1dB的雜訊指數。應該被強調的是此低雜訊放大器展現了從77.5GHz到101.5GHz之高達24GHz 3dB頻寬。另外在此論文中的兩個放大器皆使用了MMIN(最小的雜訊)技術去最佳化兩個電路的特性,並且採用了搭配基底耦合共地面波導匹配網路(GCPW-PGS) 讓兩個電路的信號損失及基底損耗降到最小。
In this thesis, two low-noise amplifiers for W-band (75-110GHz) applications are discussed regarding their design, simulation, and measurement. For the passive millimeter wave imaging (PMMW) at W-band, we propose a 94GHz LNA with and T transformers implemented in 90-nm CMOS process. By utilizing the transformer technique, the noise can be effectively suppressed; also, the input matching bandwidth can be enhanced as well. In addition, the T transformer technique is employed to reduce the loss from the series resistor in gate inductor, enhancing the performance of the LNA. The LNA achieves the power gain of 15.8dB, a minimum noise figure of 6.8 dB and moderate power consumption of 35 mW. Another LNA, a W-band LNA with coupled resonators, is also implemented in 90-nm CMOS process for W-band applications such as anti-collision radar and passive imaging. Compared with previous studies, mostly using the T matching network for W-band LNA design, this LNA proposes new coupled resonator matching network to obtain a wide 3dB bandwidth due to the provided wideband loading. Furthermore, the transformer technique is adopted to improve the overall noise performance of the LNA. The LNA achieves the power gain of 11.87dB, a minimum noise figure of 7.1 dB under a power consumption of 45 mW. It should be emphasized that the LNA obtains a very wide 3dB-bandwidth up to 24 GHz from 77.5GHz to 101.5GHz. In addition, both amplifiers use the minimum noise measure MMIN technique to optimize their performance and adopt grounded-coplanar waveguide (GCPW) structure with PGS for their minimizing signal and substrate loss.