A 5.0-to-6.36GHz Wideband-Harmonic-Shaping VCO Achieving 196.9dBc/Hz Peak FoM and 90-to-180kHz 1/f3 PN Corner Without Harmonic Tuning

Hao Guo, Yong Chen, Pui-in Mak, R. Martins
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引用次数: 22

Abstract

Since 2001 [1], LC VCOs have been demonstrating significant improvements of figureof-merit (FoM) and 1/f phase noise (PN) corner [2–5] by exploring common-mode (CM) resonance at twice the oscillation frequency $\left(2 F_{0 s c}\right)$. In addition, for area reduction, the shaping of the impulse sensitivity function (ISF) has evolved from explicit with two coils [1] to implicit with one coil [2]. Yet, as depicted in Fig. 20.1.1, the latter suffers from large CM magnetic-flux cancellation, resulting in a much lower CM impedance $\left|Z_{c M}\right|$ that is $\sim 0.64$ of its differential-mode (DM) impedance $\left|Z_{D M}\right|$. The VCO in [3] achieves a high FoM $_{\circledast 10 \mathrm{M}+\mathrm{z}}$ up to $191.4 \mathrm{dBc} / \mathrm{Hz}$ by boosting $\left|\mathrm{Z}_{\mathrm{CM}}\right|$ at $2 \mathrm{~F}_{0 \mathrm{sc}}$ and $\left|\mathrm{Z}_{\mathrm{DM}}\right|$ at $3 \mathrm{~F}_{{osc. }}$ Yet, to uphold an optimal performance over the tuning range (TR), the VCO in [3]still requires manual harmonic tuning for aligning the $1^{{st }}-t 0-2^{{nd }}$ and $1^{{st }-t 0-3^{{d }} { harmonic resonances. This }}$ denotes a narrowband effect. For the VCO in [4], which features a four-winding transformer with no harmonic tuning, there is a large variation of FoM $_{\circledast 10 \mathrm{MHz}}(190.7 \mathrm{t} \mathrm{t}$ $196.5 \mathrm{dBc} / \mathrm{Hz}$) and 1/f PN corner (60 to 600kHz) across the TR.
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一种5.0 ~ 6.36 ghz宽带谐波整形压控振荡器,实现196.9dBc/Hz峰值波形和90 ~ 180khz 1/f3 PN角
自2001年以来[1],LC压控振荡器通过在两倍振荡频率$\left(2 F_{0 s c}\right)$下探索共模(CM)共振,已经证明了性能因数(FoM)和1/f相位噪声(PN)角[2-5]的显著改进。此外,为了减小面积,脉冲灵敏度函数(ISF)的形状也从两个线圈的显式形状[1]演变为一个线圈的隐式形状[2]。然而,如图20.1.1所示,后者遭受较大的CM磁通抵消,导致CM阻抗$\left|Z_{c M}\right|$低得多,即其差模(DM)阻抗$\left|Z_{D M}\right|$的$\sim 0.64$。[3]中的VCO通过在$2 \mathrm{~F}_{0 \mathrm{sc}}$和$3 \mathrm{~F}_{{osc. }}$上分别提高$\left|\mathrm{Z}_{\mathrm{CM}}\right|$和$\left|\mathrm{Z}_{\mathrm{DM}}\right|$来实现高FoM $_{\circledast 10 \mathrm{M}+\mathrm{z}}$至$191.4 \mathrm{dBc} / \mathrm{Hz}$。然而,为了在调谐范围(TR)内保持最佳性能,[3]中的VCO仍然需要手动谐波调谐以对准$1^{{st }}-t 0-2^{{nd }}$和$1^{{st }-t 0-3^{{d }} { harmonic resonances. This }}$,这表示窄带效应。对于[4]中的VCO,其特点是没有谐波调谐的四绕组变压器,在整个TR中有很大的FoM ($_{\circledast 10 \mathrm{MHz}}(190.7 \mathrm{t} \mathrm{t}$$196.5 \mathrm{dBc} / \mathrm{Hz}$)和1/f PN角(60至600kHz)变化。
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