Subsampling PLLs (SSPLLs) are attractive architectures to generate ultra-low-jitter RF signals due to their intrinsically high phase-error-detection gain, KSH. However, this high-gain operation of a sample-and-hold circuit (SH) also has a downside that makes it difficult to achieve a fractional resolution. This is because the quantization error (Q-error) due to the non-integer relationship between the reference frequency, fREF, and the VCO frequency, f VCO , easily makes sampling points fall outside the linear range of the SH. Thus, to have a fractional resolution, SSPLLs must have a dedicated method for cancelling the Q-error. The top left of Fig. 32.4.1 shows a time-domain Q-error cancellation (TD-QEC) that is currently popular [1]. As a digital-to-time converter (DTC) cancels the Q-error, the VCO output, S VCO , can be continuously sampled at high-K SH points in the steady state. However, a critical problem is that, since the DTC is located at the front, its thermal noise cannot be suppressed by K SH degrading the in-band phase noise (PN) of SSPLLs. In contrast, in reference-sampling PLLs (RSPLLs) [2,3], the divided signal of the S VCO samples the reference clock, SREF. However, they have a fundamental limit to achieve a low jitter since their K SH is much smaller than that of SSPLLs while the thermal noise of the DTC is still high.