具有- 253.5dB抖动FOM和<-67dBc参考杂散的无分频参考采样射频锁相环

J. Sharma, H. Krishnaswamy
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引用次数: 18

摘要

最近,在无分频锁相环方面取得了令人兴奋的进展,例如子采样锁相环(sspll)[1,2]和注入锁定时钟乘法器(ilcm)[3],它们大大降低了环路噪声,从而跨越- 250dB抖动功率因数(FOM)障碍。然而,锁相环中的FOM和参考杂散之间存在一个基本的权衡,尽管机制因架构而异。窄锁相环带宽是通过滤波减少杂散所必需的,但这可能与抖动的最佳带宽相冲突。在sspll中,缓冲器将压控振荡器与次采样鉴相器(SSPD)隔离(图15.7.1),以噪声和功耗为代价减少杂散。SSPD中较小的样品电容减少了由错配引起的电荷共享、电荷注入和储罐调频产生的杂散,但代价是增加了kT/C噪声。因此,[2]的SSPLL通过使用隔离缓冲器实现了杂散<-80dBc,这是一个小的采样电容(以及另一种基于dll的技术),但显示出−244.6dB的FOM。在[1]的SSPLL中,消除该隔离缓冲并使用更大的电容会产生更好的FOM,为- 252dB,但杂散为- 56dBc。[3]中的ILCM使用大注入量来锁定参考的高倍数,但这会降低杂散。没有噪声环路元件产生一个非常低的,但大的注入导致- 43dBc的杂散。此外,ilcm没有明确的相位检测器,限制了环路动力学的优化。
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A dividerless reference-sampling RF PLL with −253.5dB jitter FOM and <-67dBc Reference Spurs
In the recent past, there have been exciting advances in dividerless PLLs, such as sub-sampling PLLs (SSPLLs) [1,2] and injection-locked clock multipliers (ILCMs) [3] that substantially reduce loop noise to cross the −250dB jitter-power figure-of-merit (FOM,) barrier. However, there exists a fundamental trade-off between FOM, and reference spurs in PLLs, although the mechanisms vary across architectures. Narrow PLL bandwidths are necessary for reducing spurs through filtering, but this can conflict with the optimal bandwidth for jitter. In SSPLLs, buffers, isolating the VCO from the sub-sampled phase detector (SSPD) (Fig. 15.7.1), reduce spurs at the expense of noise and power consumption. Smaller sample capacitances in the SSPD reduce spurs generated by mismatch-induced charge sharing, charge injection, and tank frequency modulation at the expense of increased kT/C noise. Consequently, the SSPLL of [2] achieves spur <-80dBc by using isolation buffers, a small sample capacitance (and another DLL-based technique) but exhibits an FOM, of −244.6dB. In the SSPLL of [1], the elimination of this isolation buffer and the use of a larger capacitance results in a better FOM, of −252dB but a spur of −56dBc. The ILCM in [3] operates with large injection to enable locking to a high multiple of the reference, but this degrades spurs. The absence of noisy loop components yields a very low, but large injection leads to a spur of −43dBc. Also, ILCMs do not feature explicit phase detectors, limiting the optimization of loop dynamics.
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