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A 0.049mm2 7.1-to-16.8GHz Dual-Core Triple-Mode VCO Achieving 200dB $\mathbf{FoM}_{\mathbf{A}}$ in 22nm FinFET
31
Citations
4
References
2022
Year
Electrical EngineeringEngineeringVlsi DesignPhysicsOscillatorsLow Phase NoiseHigh-frequency DeviceMixed-signal Integrated CircuitApplied PhysicsRadio FrequencyComputer EngineeringTank Quality FactorLc VcosMicroelectronicsMicrowave EngineeringFrequency ControlElectronic Circuit
LC VCOs with low phase noise (PN) and an octave frequency-tuning range (FTR) are required for multistandard communication devices, software-defined radios, and wireline data links. A viable popular approach is to exploit multicore mode-switching VCOs for two reasons: (1) their PN improves linearly by in-phase coupling of N identical VCOs; (2) the resonant-mode switching enhances the VCO FTR without degrading the tank quality factor (Q) as no RF current ideally flows through lossy mode-selection switches. However, it is still challenging for dual-mode VCOs to achieve a competitive FoM while covering an octave FTR at oscillation frequencies <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(\mathrm{F}_{\text{OSC}})$</tex> above 6GHz [1]. To enhance the number of oscillation modes to 3, [2] added a center-loop inductor <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(\mathrm{L}_{\mathrm{C}})$</tex> to a transformer, as shown in Fig. 9.2.1. However, a large FTR gap is measured, since the transformer windings should be strongly coupled to accommodate <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{L}_{\mathrm{C}}$</tex> , The authors of [3] and [4] realized a triple- and quad-mode operation, respectively, by coupling two individual transformer-based resonators (see Fig. 9.2.1). Apart from the large area penalty, the former needs an extra third winding <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(\mathrm{L}_{\mathrm{T}})$</tex> in each transformer that degrades the tank Q, while the latter used large, fixed coupling capacitors <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$(\mathrm{C}_{\mathrm{M}})$</tex> that load the tank in two of the resonant modes, thus limiting the VCO FTR.
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