在22nm FinFET中实现200dB $\mathbf{FoM}_{\mathbf{A}}$的0.049mm2 7.1至16.8 ghz双核三模压控振荡器

Jiang Gong, B. Patra, Luc Enthoven, J. V. Staveren, F. Sebastiano, M. Babaie
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引用次数: 1

摘要

具有低相位噪声(PN)和一个倍频频率调谐范围(FTR)的LC压控振荡器是多标准通信设备、软件定义无线电和有线数据链路所必需的。一种可行的流行方法是利用多核模式切换vco,有两个原因:(1)它们的PN通过N个相同的vco的同相耦合线性提高;(2)谐振模式开关提高了VCO的FTR,而不会降低槽质量因子(Q),因为没有射频电流理想地流过损耗模式选择开关。然而,对于双模vco来说,在覆盖振荡频率$(\ mathm {F}_{\text{OSC}} $高于6GHz的一个倍频FTR的同时实现具有竞争力的FoM仍然具有挑战性[1]。为了将振荡模数增加到3个,[2]在变压器上增加了一个中心环电感$(\ mathm {L}_{\ mathm {C}})$,如图9.2.1所示。然而,由于变压器绕组应该强耦合以容纳$\ mathm {L}_{\ mathm {C}}$,因此测量到较大的FTR间隙。[3]和[4]的作者通过耦合两个单独的基于变压器的谐振器,分别实现了三模和四模工作(见图9.2.1)。除了大面积损失外,前者需要在每个变压器中额外增加第三个绕组$(\ mathm {L}_{\ mathm {T}})$,从而降低油箱Q,而后者使用大型固定耦合电容器$(\ mathm {C}_{\ mathm {M}})$,将油箱负载在两个谐振模式中,从而限制了VCO的FTR。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A 0.049mm2 7.1-to-16.8GHz Dual-Core Triple-Mode VCO Achieving 200dB $\mathbf{FoM}_{\mathbf{A}}$ in 22nm FinFET
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 $(\mathrm{F}_{\text{OSC}})$ above 6GHz [1]. To enhance the number of oscillation modes to 3, [2] added a center-loop inductor $(\mathrm{L}_{\mathrm{C}})$ 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 $\mathrm{L}_{\mathrm{C}}$, 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 $(\mathrm{L}_{\mathrm{T}})$ in each transformer that degrades the tank Q, while the latter used large, fixed coupling capacitors $(\mathrm{C}_{\mathrm{M}})$ that load the tank in two of the resonant modes, thus limiting the VCO FTR.
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