Related Experiment Video
Updated: Jun 27, 2025

05:57
Characterization of SiN Integrated Optical Phased Arrays on a Wafer-Scale Test Station
Published on: April 1, 2020
8.0K
A g/I-Based Low-Power LNA for Ka-Band Applications
David Galante-Sempere1, Jeffrey Torres-Clarke1, Javier Del Pino1
1Institute for Applied Microelectronics (IUMA), Universidad de Las Palmas de Gran Canaria, 35001 Las Palmas de Gran Canaria, Spain.
Sensors (Basel, Switzerland)
|April 27, 2024
Summary
This study introduces a novel low-power low-noise amplifier (LNA) for 5G Ka-band applications. Utilizing the gm/ID methodology, it achieves excellent performance with minimal power consumption.
Area of Science:
- Electrical Engineering
- Radio Frequency (RF) and Microwave Engineering
- Semiconductor Device Design
Background:
- The demand for high-frequency communication systems, particularly for 5G New Radio (NR) in the n257 band, necessitates efficient Low-Noise Amplifiers (LNAs).
- Traditional LNA designs often face trade-offs between power consumption, noise performance, and gain at high frequencies like Ka-band.
- The gm/ID methodology offers a promising approach for optimizing transistor performance in moderate inversion, crucial for low-power RF circuit design.
Purpose of the Study:
- To design and simulate a low-power, low-noise amplifier (LNA) optimized for Ka-band (28 GHz) 5G NR applications.
- To apply the gm/ID methodology at high frequencies (Ka-band) for the first time, exploring its benefits in RF/MW scenarios.
- To achieve a high figure of merit (FoM) by balancing gain, noise figure, and power consumption.
Main Methods:
- Implementation of a cascode LNA architecture using 45 nm silicon-on-insulator (SOI) technology.
- Application of the gm/ID methodology to optimize transistor operation in the moderate inversion region for enhanced efficiency.
- Post-layout simulations were conducted to evaluate circuit performance, including gain, noise figure, and return loss.
Main Results:
- The designed LNA achieves a very low power consumption of 1.98 mW from a 0.9 V supply.
- The amplifier operates at a central frequency of 28 GHz, suitable for the 5G NR n257 band.
- Post-layout simulations show a gain of 11.4 dB, a noise figure (NF) of 3.8 dB, and an input return loss (IRL) better than 12 dB.
- The design demonstrates a remarkable figure of merit (FoM) compared to conventional approaches, with performance metrics comparable to other designs but with significantly lower power usage.
Conclusions:
- The gm/ID methodology is effectively applied to a Ka-band LNA design, demonstrating its viability at high frequencies.
- The proposed LNA offers a competitive solution for 5G Ka-band applications requiring high performance and ultra-low power consumption.
- This design contributes to the advancement of efficient RF front-end components for next-generation wireless communication systems.
Related Concept Videos
Inductively Coupled Plasma Atomic Emission Spectroscopy: Instrumentation
213
Inductively coupled plasma (ICP) is the common plasma source used in atomic emission spectroscopy (AES), a technique that detects and analyzes various elements in a sample. This method is often called inductively coupled plasma atomic emission spectroscopy (ICP-AES).
There are three main types of inductively coupled plasma atomic emission spectroscopy (ICP-AES) instruments: sequential, simultaneous multichannel, and Fourier transform instruments, with the latter being less commonly used....
There are three main types of inductively coupled plasma atomic emission spectroscopy (ICP-AES) instruments: sequential, simultaneous multichannel, and Fourier transform instruments, with the latter being less commonly used....
213
Active Filters
823
Active filters are electronic circuits that use operational amplifiers (op-amps), resistors, and capacitors to filter out unwanted frequency components from a signal. A first-order low-pass active filter is designed to pass signals with a frequency lower than a certain cutoff frequency and attenuate frequencies higher than that cutoff frequency. The transfer function for a first-order low-pass active filter is:
823

