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32.4 A 104fsrms-Jitter and -61dBc-Fractional Spur 15GHz Fractional-N Subsampling PLL Using a Voltage-Domain Quantization-Error Cancelation Technique

Author(s)
Kim, J.Jo, Y.Lim, Y.Seong, T.Park, H.Yoo, S.Lee, Y.Choi, S.Choi, J.
Issued Date
2021-02-13
DOI
10.1109/ISSCC42613.2021.9365815
URI
https://scholarworks.unist.ac.kr/handle/201301/77623
Citation
2021 IEEE International Solid-State Circuits Conference, ISSCC 2021, pp.448 - 450
Abstract
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, fVCO, 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, SVCO, can be continuously sampled at high-KSH 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 KSH degrading the in-band phase noise (PN) of SSPLLs. In contrast, in reference-sampling PLLs (RSPLLs) [2], [3], the divided signal of the SVCO samples the reference clock, S_{REF.} However, they have a fundamental limit to achieve a low jitter since their KSH is much smaller than that of SSPLLs while the thermal noise of the DTC is still high. © 2021 IEEE.
Publisher
Institute of Electrical and Electronics Engineers Inc.
ISSN
0193-6530

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