2010
DOI: 10.1017/s1759078710000395
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A highly efficient 3.5 GHz inverse class-F GaN HEMT power amplifier

Abstract: This paper presents the design and implementation of an inverse class-F power amplifier (PA) using a high power gallium nitride high electron mobility transistor (GaN HEMT). For a 3.5 GHz continuous wave signal, the measurement results show state-of-the-art power-added efficiency (PAE) of 78%, a drain efficiency of 82%, a gain of 12 dB, and an output power of 12 W. Moreover, over a 300 MHz bandwidth, the PAE and output power are maintained at 60% and 10 W, respectively. Linearized modulated measurements using … Show more

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Cited by 14 publications
(12 citation statements)
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“…Although good agreement between simulation and measurement results are obtained, the discrepancy at high power may be related to the self-heating in the device. At low output power, the differences between simulated and measured performance may be related to the switch mode operation of the model [26][27][28].…”
Section: Cw Performancementioning
confidence: 99%
“…Although good agreement between simulation and measurement results are obtained, the discrepancy at high power may be related to the self-heating in the device. At low output power, the differences between simulated and measured performance may be related to the switch mode operation of the model [26][27][28].…”
Section: Cw Performancementioning
confidence: 99%
“…Measurements were then performed using the class F −1 PA published in [13]. This PA has a peak power added efficiency (PAE) of 78% at 3.5 GHz.…”
Section: A Prerequisitesmentioning
confidence: 99%
“…Fig. 9 shows such an example where a static power sweep performed on a class F −1 GaN amplifier [27] is used, in combination with an SNR calculation based on simulation using a data record of 10 6 samples generated as stated in the prerequisites. The result is compared to the ideal class B based efficiency estimate, η B from (37), and the SNR estimate, SNR est from (42).…”
Section: B Simulationsmentioning
confidence: 99%
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“…Other than the optimum fundamental terminations, the optimum magnitudes of the higher harmonic reflection coefficients are typically near to unity with different phases depending on the P A classes, e.g. class-J [2], class-F or inverse class-F [4][5]. With passive tuner setups these high reflection conditions equal to unity cannot be set due to losses introduced by the various components such as couplers, diplexers, cables and probes.…”
Section: Introductionmentioning
confidence: 99%