Jiang Gong, B. Patra, Luc Enthoven, J. V. Staveren, F. Sebastiano, M. Babaie
{"title":"在22nm FinFET中实现200dB $\\mathbf{FoM}_{\\mathbf{A}}$的0.049mm2 7.1至16.8 ghz双核三模压控振荡器","authors":"Jiang Gong, B. Patra, Luc Enthoven, J. V. Staveren, F. Sebastiano, M. Babaie","doi":"10.1109/ISSCC42614.2022.9731752","DOIUrl":null,"url":null,"abstract":"LC VCOs with low phase noise (PN) and an octave frequency-tuning range (FTR) are required for multistandard communication devices, software-defined radios, and wireline data links. A viable popular approach is to exploit multicore mode-switching VCOs for two reasons: (1) their PN improves linearly by in-phase coupling of N identical VCOs; (2) the resonant-mode switching enhances the VCO FTR without degrading the tank quality factor (Q) as no RF current ideally flows through lossy mode-selection switches. However, it is still challenging for dual-mode VCOs to achieve a competitive FoM while covering an octave FTR at oscillation frequencies $(\\mathrm{F}_{\\text{OSC}})$ above 6GHz [1]. To enhance the number of oscillation modes to 3, [2] added a center-loop inductor $(\\mathrm{L}_{\\mathrm{C}})$ to a transformer, as shown in Fig. 9.2.1. However, a large FTR gap is measured, since the transformer windings should be strongly coupled to accommodate $\\mathrm{L}_{\\mathrm{C}}$, The authors of [3] and [4] realized a triple- and quad-mode operation, respectively, by coupling two individual transformer-based resonators (see Fig. 9.2.1). Apart from the large area penalty, the former needs an extra third winding $(\\mathrm{L}_{\\mathrm{T}})$ in each transformer that degrades the tank Q, while the latter used large, fixed coupling capacitors $(\\mathrm{C}_{\\mathrm{M}})$ that load the tank in two of the resonant modes, thus limiting the VCO FTR.","PeriodicalId":6830,"journal":{"name":"2022 IEEE International Solid- State Circuits Conference (ISSCC)","volume":"23 1","pages":"1-3"},"PeriodicalIF":0.0000,"publicationDate":"2022-02-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"A 0.049mm2 7.1-to-16.8GHz Dual-Core Triple-Mode VCO Achieving 200dB $\\\\mathbf{FoM}_{\\\\mathbf{A}}$ in 22nm FinFET\",\"authors\":\"Jiang Gong, B. Patra, Luc Enthoven, J. V. Staveren, F. Sebastiano, M. Babaie\",\"doi\":\"10.1109/ISSCC42614.2022.9731752\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"LC VCOs with low phase noise (PN) and an octave frequency-tuning range (FTR) are required for multistandard communication devices, software-defined radios, and wireline data links. A viable popular approach is to exploit multicore mode-switching VCOs for two reasons: (1) their PN improves linearly by in-phase coupling of N identical VCOs; (2) the resonant-mode switching enhances the VCO FTR without degrading the tank quality factor (Q) as no RF current ideally flows through lossy mode-selection switches. However, it is still challenging for dual-mode VCOs to achieve a competitive FoM while covering an octave FTR at oscillation frequencies $(\\\\mathrm{F}_{\\\\text{OSC}})$ above 6GHz [1]. To enhance the number of oscillation modes to 3, [2] added a center-loop inductor $(\\\\mathrm{L}_{\\\\mathrm{C}})$ to a transformer, as shown in Fig. 9.2.1. However, a large FTR gap is measured, since the transformer windings should be strongly coupled to accommodate $\\\\mathrm{L}_{\\\\mathrm{C}}$, The authors of [3] and [4] realized a triple- and quad-mode operation, respectively, by coupling two individual transformer-based resonators (see Fig. 9.2.1). Apart from the large area penalty, the former needs an extra third winding $(\\\\mathrm{L}_{\\\\mathrm{T}})$ in each transformer that degrades the tank Q, while the latter used large, fixed coupling capacitors $(\\\\mathrm{C}_{\\\\mathrm{M}})$ that load the tank in two of the resonant modes, thus limiting the VCO FTR.\",\"PeriodicalId\":6830,\"journal\":{\"name\":\"2022 IEEE International Solid- State Circuits Conference (ISSCC)\",\"volume\":\"23 1\",\"pages\":\"1-3\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2022-02-20\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2022 IEEE International Solid- State Circuits Conference (ISSCC)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ISSCC42614.2022.9731752\",\"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/ISSCC42614.2022.9731752","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A 0.049mm2 7.1-to-16.8GHz Dual-Core Triple-Mode VCO Achieving 200dB $\mathbf{FoM}_{\mathbf{A}}$ in 22nm FinFET
LC VCOs with low phase noise (PN) and an octave frequency-tuning range (FTR) are required for multistandard communication devices, software-defined radios, and wireline data links. A viable popular approach is to exploit multicore mode-switching VCOs for two reasons: (1) their PN improves linearly by in-phase coupling of N identical VCOs; (2) the resonant-mode switching enhances the VCO FTR without degrading the tank quality factor (Q) as no RF current ideally flows through lossy mode-selection switches. However, it is still challenging for dual-mode VCOs to achieve a competitive FoM while covering an octave FTR at oscillation frequencies $(\mathrm{F}_{\text{OSC}})$ above 6GHz [1]. To enhance the number of oscillation modes to 3, [2] added a center-loop inductor $(\mathrm{L}_{\mathrm{C}})$ to a transformer, as shown in Fig. 9.2.1. However, a large FTR gap is measured, since the transformer windings should be strongly coupled to accommodate $\mathrm{L}_{\mathrm{C}}$, The authors of [3] and [4] realized a triple- and quad-mode operation, respectively, by coupling two individual transformer-based resonators (see Fig. 9.2.1). Apart from the large area penalty, the former needs an extra third winding $(\mathrm{L}_{\mathrm{T}})$ in each transformer that degrades the tank Q, while the latter used large, fixed coupling capacitors $(\mathrm{C}_{\mathrm{M}})$ that load the tank in two of the resonant modes, thus limiting the VCO FTR.