Suneui Park, Seyeon Yoo, Yuhwan Shin, Jeonghyun Lee, Jaehyouk Choi
{"title":"具有功率门控注入锁定和背景多功能数字校准器的8.16GHz环形振荡器注入锁定时钟乘法器","authors":"Suneui Park, Seyeon Yoo, Yuhwan Shin, Jeonghyun Lee, Jaehyouk Choi","doi":"10.1109/ISSCC42614.2022.9731713","DOIUrl":null,"url":null,"abstract":"To generate low-jitter, high-frequency signals with ring oscillators (ROs), injection-locked clock multipliers (ILCMs) are the most suitable architecture due to advantages such wide bandwidth and fewer noise sources. However, they have two inherent issues. The first is that their jitter performance is sensitive to PVT variations. To address this problem, recent RO-ILCMs have been equipped with a multi-purpose, real-time digital calibrator that can remove both the frequency error of the RO and the phase error of the calibrator [1]–[2]. The second is that their operational stability and jitter performance degrade rapidly as the multiplication factor, N, increases. This issue, which has yet to be well addressed, is rooted in the fundamental limitation of the typical injection-locking method, i.e., injecting narrow pulses into the RO (top left of Fig. 13.2.1). When the free-running frequency of the RO deviates from the target frequency, $Nf_{\\text{REF}}$, where $f_{\\text{REF}}$ is the frequency of the reference clock $(\\mathcal{S}_{\\text{REF}})$, the core current of the RO $(I_{\\text{osc}})$ and the $\\text{injecting}$ current $(I_{\\text{INJ}})$ should be out of phase to satisfy the oscillation condition by creating the necessary phase shift. Thus, the effective magnitude of $I_{\\text{INJ}}$ at $N f_{\\text {REF, }} \\text {i.e}., I_{\\text{INJ,eff }}$, relative to $l_{\\text{osc}}$ determines the maximum phase angle, $\\phi_{\\text{MAX}}$, and, thus, the maximum lock range, $\\omega_{\\mathrm{L},\\text{MAX}}$ [3]. However, for a large $N, I_{\\text{INJ,eff} }$ becomes extremely small, sharply reducing $\\phi_{\\text{MAX}}$ and $\\omega_{\\mathrm{L},\\text{MAX}}$. Although the RO-ILCMs in [4]–[5] achieved a total $N$ of over 40 by using a reference doubler or quadrupler, their two-stage operation offers limited improvement of the jitter $\\text{FoM}$. MDLL-based implementations are better suited for larger N, but the time required for edge switching limits the maximum output frequency, $f_{\\text{OUT}}$, and the value of N.","PeriodicalId":6830,"journal":{"name":"2022 IEEE International Solid- State Circuits Conference (ISSCC)","volume":"36 1","pages":"1-3"},"PeriodicalIF":0.0000,"publicationDate":"2022-02-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":"{\"title\":\"A 97fsrms-Jitter and 68-Multiplication Factor, 8.16GHz Ring-Oscillator Injection-Locked Clock Multiplier with Power-Gating Injection-Locking and Background Multi-Functional Digital Calibrator\",\"authors\":\"Suneui Park, Seyeon Yoo, Yuhwan Shin, Jeonghyun Lee, Jaehyouk Choi\",\"doi\":\"10.1109/ISSCC42614.2022.9731713\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"To generate low-jitter, high-frequency signals with ring oscillators (ROs), injection-locked clock multipliers (ILCMs) are the most suitable architecture due to advantages such wide bandwidth and fewer noise sources. However, they have two inherent issues. The first is that their jitter performance is sensitive to PVT variations. To address this problem, recent RO-ILCMs have been equipped with a multi-purpose, real-time digital calibrator that can remove both the frequency error of the RO and the phase error of the calibrator [1]–[2]. The second is that their operational stability and jitter performance degrade rapidly as the multiplication factor, N, increases. This issue, which has yet to be well addressed, is rooted in the fundamental limitation of the typical injection-locking method, i.e., injecting narrow pulses into the RO (top left of Fig. 13.2.1). When the free-running frequency of the RO deviates from the target frequency, $Nf_{\\\\text{REF}}$, where $f_{\\\\text{REF}}$ is the frequency of the reference clock $(\\\\mathcal{S}_{\\\\text{REF}})$, the core current of the RO $(I_{\\\\text{osc}})$ and the $\\\\text{injecting}$ current $(I_{\\\\text{INJ}})$ should be out of phase to satisfy the oscillation condition by creating the necessary phase shift. Thus, the effective magnitude of $I_{\\\\text{INJ}}$ at $N f_{\\\\text {REF, }} \\\\text {i.e}., I_{\\\\text{INJ,eff }}$, relative to $l_{\\\\text{osc}}$ determines the maximum phase angle, $\\\\phi_{\\\\text{MAX}}$, and, thus, the maximum lock range, $\\\\omega_{\\\\mathrm{L},\\\\text{MAX}}$ [3]. However, for a large $N, I_{\\\\text{INJ,eff} }$ becomes extremely small, sharply reducing $\\\\phi_{\\\\text{MAX}}$ and $\\\\omega_{\\\\mathrm{L},\\\\text{MAX}}$. Although the RO-ILCMs in [4]–[5] achieved a total $N$ of over 40 by using a reference doubler or quadrupler, their two-stage operation offers limited improvement of the jitter $\\\\text{FoM}$. MDLL-based implementations are better suited for larger N, but the time required for edge switching limits the maximum output frequency, $f_{\\\\text{OUT}}$, and the value of N.\",\"PeriodicalId\":6830,\"journal\":{\"name\":\"2022 IEEE International Solid- State Circuits Conference (ISSCC)\",\"volume\":\"36 1\",\"pages\":\"1-3\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2022-02-20\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"4\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2022 IEEE International Solid- State Circuits Conference (ISSCC)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ISSCC42614.2022.9731713\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2022 IEEE International Solid- State Circuits Conference (ISSCC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ISSCC42614.2022.9731713","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A 97fsrms-Jitter and 68-Multiplication Factor, 8.16GHz Ring-Oscillator Injection-Locked Clock Multiplier with Power-Gating Injection-Locking and Background Multi-Functional Digital Calibrator
To generate low-jitter, high-frequency signals with ring oscillators (ROs), injection-locked clock multipliers (ILCMs) are the most suitable architecture due to advantages such wide bandwidth and fewer noise sources. However, they have two inherent issues. The first is that their jitter performance is sensitive to PVT variations. To address this problem, recent RO-ILCMs have been equipped with a multi-purpose, real-time digital calibrator that can remove both the frequency error of the RO and the phase error of the calibrator [1]–[2]. The second is that their operational stability and jitter performance degrade rapidly as the multiplication factor, N, increases. This issue, which has yet to be well addressed, is rooted in the fundamental limitation of the typical injection-locking method, i.e., injecting narrow pulses into the RO (top left of Fig. 13.2.1). When the free-running frequency of the RO deviates from the target frequency, $Nf_{\text{REF}}$, where $f_{\text{REF}}$ is the frequency of the reference clock $(\mathcal{S}_{\text{REF}})$, the core current of the RO $(I_{\text{osc}})$ and the $\text{injecting}$ current $(I_{\text{INJ}})$ should be out of phase to satisfy the oscillation condition by creating the necessary phase shift. Thus, the effective magnitude of $I_{\text{INJ}}$ at $N f_{\text {REF, }} \text {i.e}., I_{\text{INJ,eff }}$, relative to $l_{\text{osc}}$ determines the maximum phase angle, $\phi_{\text{MAX}}$, and, thus, the maximum lock range, $\omega_{\mathrm{L},\text{MAX}}$ [3]. However, for a large $N, I_{\text{INJ,eff} }$ becomes extremely small, sharply reducing $\phi_{\text{MAX}}$ and $\omega_{\mathrm{L},\text{MAX}}$. Although the RO-ILCMs in [4]–[5] achieved a total $N$ of over 40 by using a reference doubler or quadrupler, their two-stage operation offers limited improvement of the jitter $\text{FoM}$. MDLL-based implementations are better suited for larger N, but the time required for edge switching limits the maximum output frequency, $f_{\text{OUT}}$, and the value of N.