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  • Print publication year: 2016
  • Online publication date: April 2016

4 - Linear-mode mm-wave silicon power amplifiers


Why linear?

Two fundamental questions arise in the design of a power amplifier circuit. First, what is the maximum output power given a device technology? Second, what is the peak power-added efficiency (PAE) given a device technology? In this chapter, these fundamental limits on output power and efficiency are analyzed for single-stage, linear millimeter-wave (mm-wave) PAs based on device and circuit factors. Linear amplifiers are favored under several conditions. Foremost, a linear response might be demanded for complex signaling. Quadrature amplitude modulation (QAM) requires a linear response to support the peak-to-average power ratio (PAPR) of the signal envelope. As shown in Fig. 4.1, the in-phase and quadrature symbols – shown as a 64QAM constellation – are up-converted to an RF carrier and amplified by the power amplifier. The envelope of the modulated RF signal is shown at the output of the PA and demonstrates substantial variation in the output power. The ratio of the peak-to-average power indicates the linearity requirements of the power amplifier. Additionally, concerns about the out-of-channel interference, e.g. spectral leakage, also dictate requirements for system linearity. However, specification of adjacent channel interference is not well-established at mm-wave bands since the spatial selectivity of the communication system at these bands is considered to be higher than for RF systems.

In RF systems, linear amplifiers are rarely sufficiently linear and additional linearization can be introduced in the form of feedforward, feedback, or digital pre-distortion. The evolution of communication standards tends to favor more spectrally efficient communication and, in turn, motivates interest in linearization techniques for power amplifiers. In the case of mm-wave communication, early commercial standards have avoided the need for linear amplifiers by using constant envelope waveforms such as GMSK or simple modulation schemes that feature low PAPR such as QPSK. As more interest develops in mm-wave QAM, circuit and system techniques that offer a linear variation in the output power will return to the forefront.

A second motivation for linear amplifier designs is that this class of operation may offer competitive output power and efficiency at mm-wave bands to other classes of amplifiers. For instance, switching amplifiers require harmonic control that complicates the design of these amplifiers over wide bandwidth at mm-wave bands. Another desirable feature of linear amplifiers is that two PAs can be configured to be maximally efficient at both the average and peak power levels.

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