1,477 research outputs found

    Attosecond Precision Multi-km Laser-Microwave Network

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    Synchronous laser-microwave networks delivering attosecond timing precision are highly desirable in many advanced applications, such as geodesy, very-long-baseline interferometry, high-precision navigation and multi-telescope arrays. In particular, rapidly expanding photon science facilities like X-ray free-electron lasers and intense laser beamlines require system-wide attosecond-level synchronization of dozens of optical and microwave signals up to kilometer distances. Once equipped with such precision, these facilities will initiate radically new science by shedding light on molecular and atomic processes happening on the attosecond timescale, such as intramolecular charge transfer, Auger processes and their impact on X-ray imaging. Here, we present for the first time a complete synchronous laser-microwave network with attosecond precision, which is achieved through new metrological devices and careful balancing of fiber nonlinearities and fundamental noise contributions. We demonstrate timing stabilization of a 4.7-km fiber network and remote optical-optical synchronization across a 3.5-km fiber link with an overall timing jitter of 580 and 680 attoseconds RMS, respectively, for over 40 hours. Ultimately we realize a complete laser-microwave network with 950-attosecond timing jitter for 18 hours. This work can enable next-generation attosecond photon-science facilities to revolutionize many research fields from structural biology to material science and chemistry to fundamental physics.Comment: 42 pages, 13 figure

    Numerical investigation of a feed-forward linewidth reduction scheme using a mode-locked laser model of reduced complexity

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    We provide numerical verification of a feed-forward, heterodyne-based phase noise reduction scheme using single-sideband modulation that obviates the need for optical filtering at the output. The main benefit of a feed-forward heterodyne linewidth reduction scheme is the simultaneous reduction of the linewidth of all modes of a mode-locked laser (MLL) to that of a narrow-linewidth single-wavelength laser. At the heart of our simulator is an MLL model of reduced complexity. Importantly, the main issue being treated is the jitter of MLLs and we show how to create numerical waveforms that mimic the random-walk nature of timing jitter of pulses from MLLs. Thus, the model does not need to solve stochastic differential equations that describe the MLL dynamics, and the model calculates self-consistently the line-broadening of the modes of the MLL and shows good agreement with both the optical linewidth and jitter. The linewidth broadening of the MLL modes are calculated after the phase noise reduction scheme and we confirm that the phase noise contribution from the timing jitter still remains. Finally, we use the MLL model and phase noise reduction simulator within an optical communications system simulator and show that the phase noise reduction technique could enable MLLs as optical carriers for higher-order modulation formats, such as 16-state and 64-state quadrature amplitude modulation

    Versatile Digital GHz Phase Lock for External Cavity Diode Lasers

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    We present a versatile, inexpensive and simple optical phase lock for applications in atomic physics experiments. Thanks to all-digital phase detection and implementation of beat frequency pre-scaling, the apparatus requires no microwave-range reference input, and permits phase locking at frequency differences ranging from sub-MHz to 7 GHz (and with minor extension, to 12 GHz). The locking range thus covers ground state hyperfine splittings of all alkali metals, which makes this system a universal tool for many experiments on coherent interaction between light and atoms.Comment: 4.5 pages, 5 figures v3: fixed error in schematic: R10 connects to other end of C

    ๊ณ ์† ์‹œ๋ฆฌ์–ผ ๋งํฌ๋ฅผ ์œ„ํ•œ ๊ณ ๋ฆฌ ๋ฐœ์ง„๊ธฐ๋ฅผ ๊ธฐ๋ฐ˜์œผ๋กœ ํ•˜๋Š” ์ฃผํŒŒ์ˆ˜ ํ•ฉ์„ฑ๊ธฐ

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    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2022. 8. ์ •๋•๊ท .In this dissertation, major concerns in the clocking of modern serial links are discussed. As sub-rate, multi-standard architectures are becoming predominant, the conventional clocking methodology seems to necessitate innovation in terms of low-cost implementation. Frequency synthesis with active, inductor-less oscillators replacing LC counterparts are reviewed, and solutions for two major drawbacks are proposed. Each solution is verified by prototype chip design, giving a possibility that the inductor-less oscillator may become a proper candidate for future high-speed serial links. To mitigate the high flicker noise of a high-frequency ring oscillator (RO), a reference multiplication technique that effectively extends the bandwidth of the following all-digital phase-locked loop (ADPLL) is proposed. The technique avoids any jitter accumulation, generating a clean mid-frequency clock, overall achieving high jitter performance in conjunction with the ADPLL. Timing constraint for the proper reference multiplication is first analyzed to determine the calibration points that may correct the existent phase errors. The weight for each calibration point is updated by the proposed a priori probability-based least-mean-square (LMS) algorithm. To minimize the time required for the calibration, each gain for the weight update is adaptively varied by deducing a posteriori which error source dominates the others. The prototype chip is fabricated in a 40-nm CMOS technology, and its measurement results verify the low-jitter, high-frequency clock generation with fast calibration settling. The presented work achieves an rms jitter of 177/223 fs at 8/16-GHz output, consuming 12.1/17-mW power. As the second embodiment, an RO-based ADPLL with an analog technique that addresses the high supply sensitivity of the RO is presented. Unlike prior arts, the circuit for the proposed technique does not extort the RO voltage headroom, allowing high-frequency oscillation. Further, the performance given from the technique is robust over process, voltage, and temperature (PVT) variations, avoiding the use of additional calibration hardware. Lastly, a comprehensive analysis of phase noise contribution is conducted for the overall ADPLL, followed by circuit optimizations, to retain the low-jitter output. Implemented in a 40-nm CMOS technology, the frequency synthesizer achieves an rms jitter of 289 fs at 8 GHz output without any injected supply noise. Under a 20-mVrms white supply noise, the ADPLL suppresses supply-noise-induced jitter by -23.8 dB.๋ณธ ๋…ผ๋ฌธ์€ ํ˜„๋Œ€ ์‹œ๋ฆฌ์–ผ ๋งํฌ์˜ ํด๋ฝํ‚น์— ๊ด€์—ฌ๋˜๋Š” ์ฃผ์š”ํ•œ ๋ฌธ์ œ๋“ค์— ๋Œ€ํ•˜์—ฌ ๊ธฐ์ˆ ํ•œ๋‹ค. ์ค€์†๋„, ๋‹ค์ค‘ ํ‘œ์ค€ ๊ตฌ์กฐ๋“ค์ด ์ฑ„ํƒ๋˜๊ณ  ์žˆ๋Š” ์ถ”์„ธ์— ๋”ฐ๋ผ, ๊ธฐ์กด์˜ ํด๋ผํ‚น ๋ฐฉ๋ฒ•์€ ๋‚ฎ์€ ๋น„์šฉ์˜ ๊ตฌํ˜„์˜ ๊ด€์ ์—์„œ ์ƒˆ๋กœ์šด ํ˜์‹ ์„ ํ•„์š”๋กœ ํ•œ๋‹ค. LC ๊ณต์ง„๊ธฐ๋ฅผ ๋Œ€์‹ ํ•˜์—ฌ ๋Šฅ๋™ ์†Œ์ž ๋ฐœ์ง„๊ธฐ๋ฅผ ์‚ฌ์šฉํ•œ ์ฃผํŒŒ์ˆ˜ ํ•ฉ์„ฑ์— ๋Œ€ํ•˜์—ฌ ์•Œ์•„๋ณด๊ณ , ์ด์— ๋ฐœ์ƒํ•˜๋Š” ๋‘๊ฐ€์ง€ ์ฃผ์š” ๋ฌธ์ œ์ ๊ณผ ๊ฐ๊ฐ์— ๋Œ€ํ•œ ํ•ด๊ฒฐ ๋ฐฉ์•ˆ์„ ํƒ์ƒ‰ํ•œ๋‹ค. ๊ฐ ์ œ์•ˆ ๋ฐฉ๋ฒ•์„ ํ”„๋กœํ† ํƒ€์ž… ์นฉ์„ ํ†ตํ•ด ๊ทธ ํšจ์šฉ์„ฑ์„ ๊ฒ€์ฆํ•˜๊ณ , ์ด์–ด์„œ ๋Šฅ๋™ ์†Œ์ž ๋ฐœ์ง„๊ธฐ๊ฐ€ ๋ฏธ๋ž˜์˜ ๊ณ ์† ์‹œ๋ฆฌ์–ผ ๋งํฌ์˜ ํด๋ฝํ‚น์— ์‚ฌ์šฉ๋  ๊ฐ€๋Šฅ์„ฑ์— ๋Œ€ํ•ด ๊ฒ€ํ† ํ•œ๋‹ค. ์ฒซ๋ฒˆ์งธ ์‹œ์—ฐ์œผ๋กœ์จ, ๊ณ ์ฃผํŒŒ ๊ณ ๋ฆฌ ๋ฐœ์ง„๊ธฐ์˜ ๋†’์€ ํ”Œ๋ฆฌ์ปค ์žก์Œ์„ ์™„ํ™”์‹œํ‚ค๊ธฐ ์œ„ํ•ด ๊ธฐ์ค€ ์‹ ํ˜ธ๋ฅผ ๋ฐฐ์ˆ˜ํ™”ํ•˜์—ฌ ๋’ท๋‹จ์˜ ์œ„์ƒ ๊ณ ์ • ๋ฃจํ”„์˜ ๋Œ€์—ญํญ์„ ํšจ๊ณผ์ ์œผ๋กœ ๊ทน๋Œ€ํ™” ์‹œํ‚ค๋Š” ํšŒ๋กœ ๊ธฐ์ˆ ์„ ์ œ์•ˆํ•œ๋‹ค. ๋ณธ ๊ธฐ์ˆ ์€ ์ง€ํ„ฐ๋ฅผ ๋ˆ„์  ์‹œํ‚ค์ง€ ์•Š์œผ๋ฉฐ ๋”ฐ๋ผ์„œ ๊นจ๋—ํ•œ ์ค‘๊ฐ„ ์ฃผํŒŒ์ˆ˜ ํด๋ฝ์„ ์ƒ์„ฑ์‹œ์ผœ ์œ„์ƒ ๊ณ ์ • ๋ฃจํ”„์™€ ํ•จ๊ป˜ ๋†’์€ ์„ฑ๋Šฅ์˜ ๊ณ ์ฃผํŒŒ ํด๋ฝ์„ ํ•ฉ์„ฑํ•œ๋‹ค. ๊ธฐ์ค€ ์‹ ํ˜ธ๋ฅผ ์„ฑ๊ณต์ ์œผ๋กœ ๋ฐฐ์ˆ˜ํ™”ํ•˜๊ธฐ ์œ„ํ•œ ํƒ€์ด๋ฐ ์กฐ๊ฑด๋“ค์„ ๋จผ์ € ๋ถ„์„ํ•˜์—ฌ ํƒ€์ด๋ฐ ์˜ค๋ฅ˜๋ฅผ ์ œ๊ฑฐํ•˜๊ธฐ ์œ„ํ•œ ๋ฐฉ๋ฒ•๋ก ์„ ํŒŒ์•…ํ•œ๋‹ค. ๊ฐ ๊ต์ • ์ค‘๋Ÿ‰์€ ์—ฐ์—ญ์  ํ™•๋ฅ ์„ ๊ธฐ๋ฐ˜์œผ๋กœํ•œ LMS ์•Œ๊ณ ๋ฆฌ์ฆ˜์„ ํ†ตํ•ด ๊ฐฑ์‹ ๋˜๋„๋ก ์„ค๊ณ„๋œ๋‹ค. ๊ต์ •์— ํ•„์š”ํ•œ ์‹œ๊ฐ„์„ ์ตœ์†Œํ™” ํ•˜๊ธฐ ์œ„ํ•˜์—ฌ, ๊ฐ ๊ต์ • ์ด๋“์€ ํƒ€์ด๋ฐ ์˜ค๋ฅ˜ ๊ทผ์›๋“ค์˜ ํฌ๊ธฐ๋ฅผ ๊ท€๋‚ฉ์ ์œผ๋กœ ์ถ”๋ก ํ•œ ๊ฐ’์„ ๋ฐ”ํƒ•์œผ๋กœ ์ง€์†์ ์œผ๋กœ ์ œ์–ด๋œ๋‹ค. 40-nm CMOS ๊ณต์ •์œผ๋กœ ๊ตฌํ˜„๋œ ํ”„๋กœํ† ํƒ€์ž… ์นฉ์˜ ์ธก์ •์„ ํ†ตํ•ด ์ €์†Œ์Œ, ๊ณ ์ฃผํŒŒ ํด๋ฝ์„ ๋น ๋ฅธ ๊ต์ • ์‹œ๊ฐ„์•ˆ์— ํ•ฉ์„ฑํ•ด ๋ƒ„์„ ํ™•์ธํ•˜์˜€๋‹ค. ์ด๋Š” 177/223 fs์˜ rms ์ง€ํ„ฐ๋ฅผ ๊ฐ€์ง€๋Š” 8/16 GHz์˜ ํด๋ฝ์„ ์ถœ๋ ฅํ•œ๋‹ค. ๋‘๋ฒˆ์งธ ์‹œ์—ฐ์œผ๋กœ์จ, ๊ณ ๋ฆฌ ๋ฐœ์ง„๊ธฐ์˜ ๋†’์€ ์ „์› ๋…ธ์ด์ฆˆ ์˜์กด์„ฑ์„ ์™„ํ™”์‹œํ‚ค๋Š” ๊ธฐ์ˆ ์ด ํฌํ•จ๋œ ์ฃผํŒŒ์ˆ˜ ํ•ฉ์„ฑ๊ธฐ๊ฐ€ ์„ค๊ณ„๋˜์—ˆ๋‹ค. ์ด๋Š” ๊ณ ๋ฆฌ ๋ฐœ์ง„๊ธฐ์˜ ์ „์•• ํ—ค๋“œ๋ฃธ์„ ๋ณด์กดํ•จ์œผ๋กœ์„œ ๊ณ ์ฃผํŒŒ ๋ฐœ์ง„์„ ๊ฐ€๋Šฅํ•˜๊ฒŒ ํ•œ๋‹ค. ๋‚˜์•„๊ฐ€, ์ „์› ๋…ธ์ด์ฆˆ ๊ฐ์†Œ ์„ฑ๋Šฅ์€ ๊ณต์ •, ์ „์••, ์˜จ๋„ ๋ณ€๋™์— ๋Œ€ํ•˜์—ฌ ๋ฏผ๊ฐํ•˜์ง€ ์•Š์œผ๋ฉฐ, ๋”ฐ๋ผ์„œ ์ถ”๊ฐ€์ ์ธ ๊ต์ • ํšŒ๋กœ๋ฅผ ํ•„์š”๋กœ ํ•˜์ง€ ์•Š๋Š”๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ, ์œ„์ƒ ๋…ธ์ด์ฆˆ์— ๋Œ€ํ•œ ํฌ๊ด„์  ๋ถ„์„๊ณผ ํšŒ๋กœ ์ตœ์ ํ™”๋ฅผ ํ†ตํ•˜์—ฌ ์ฃผํŒŒ์ˆ˜ ํ•ฉ์„ฑ๊ธฐ์˜ ์ €์žก์Œ ์ถœ๋ ฅ์„ ๋ฐฉํ•ดํ•˜์ง€ ์•Š๋Š” ๋ฐฉ๋ฒ•์„ ๊ณ ์•ˆํ•˜์˜€๋‹ค. ํ•ด๋‹น ํ”„๋กœํ† ํƒ€์ž… ์นฉ์€ 40-nm CMOS ๊ณต์ •์œผ๋กœ ๊ตฌํ˜„๋˜์—ˆ์œผ๋ฉฐ, ์ „์› ๋…ธ์ด์ฆˆ๊ฐ€ ์ธ๊ฐ€๋˜์ง€ ์•Š์€ ์ƒํƒœ์—์„œ 289 fs์˜ rms ์ง€ํ„ฐ๋ฅผ ๊ฐ€์ง€๋Š” 8 GHz์˜ ํด๋ฝ์„ ์ถœ๋ ฅํ•œ๋‹ค. ๋˜ํ•œ, 20 mVrms์˜ ์ „์› ๋…ธ์ด์ฆˆ๊ฐ€ ์ธ๊ฐ€๋˜์—ˆ์„ ๋•Œ์— ์œ ๋„๋˜๋Š” ์ง€ํ„ฐ์˜ ์–‘์„ -23.8 dB ๋งŒํผ ์ค„์ด๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค.1 Introduction 1 1.1 Motivation 3 1.1.1 Clocking in High-Speed Serial Links 4 1.1.2 Multi-Phase, High-Frequency Clock Conversion 8 1.2 Dissertation Objectives 10 2 RO-Based High-Frequency Synthesis 12 2.1 Phase-Locked Loop Fundamentals 12 2.2 Toward All-Digital Regime 15 2.3 RO Design Challenges 21 2.3.1 Oscillator Phase Noise 21 2.3.2 Challenge 1: High Flicker Noise 23 2.3.3 Challenge 2: High Supply Noise Sensitivity 26 3 Filtering RO Noise 28 3.1 Introduction 28 3.2 Proposed Reference Octupler 34 3.2.1 Delay Constraint 34 3.2.2 Phase Error Calibration 38 3.2.3 Circuit Implementation 51 3.3 IL-ADPLL Implementation 55 3.4 Measurement Results 59 3.5 Summary 63 4 RO Supply Noise Compensation 69 4.1 Introduction 69 4.2 Proposed Analog Closed Loop for Supply Noise Compensation 72 4.2.1 Circuit Implementation 73 4.2.2 Frequency-Domain Analysis 76 4.2.3 Circuit Optimization 81 4.3 ADPLL Implementation 87 4.4 Measurement Results 90 4.5 Summary 98 5 Conclusions 99 A Notes on the 8REF 102 B Notes on the ACSC 105๋ฐ•

    Exceeding octave tunable Terahertz waves with zepto-second level timing noise

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    Spectral purity of any millimeter wave (mmW) source is of the utmost interest in low-noise applications. Optical synthesis via photomixing is an attractive source for such mmWs, which usually involves expensive spectrally pure lasers with narrow linewidths approaching monochromaticity due to their inherent fabrication costs or specifications. Here, we report an alternative option for enhancing the spectral purity of inexpensive semiconductor diode lasers via a self-injection locking technique through corresponding Stokes waves from a fiber Brillouin cavity exhibiting greatly improved phase noise levels and large wavelength tunability of ~1.8 nm. We implement a system with two self-injected diode lasers on a common Brillouin cavity aimed at difference frequency generation in the mmW and THz region. We generate tunable sub-mmW (0.3 and 0.5 THz) waves by beating the self-injected two wavelength Stokes light on a uni-travelling carrier photodiode and characterize the noise performance. The sub-mmW features miniscule timing noise levels in the zepto-second (zs.Hz^-0.5) scale outperforming the state of the art dissipative Kerr soliton based micro-resonator setups while offering broader frequency tunability. These results suggest a viable inexpensive alternative for mmW sources aimed at low-noise applications featuring lab-scale footprints and rack-mounted portability while paving the way for chip-scale photonic integration.Comment: 31 page

    A Bang-Bang All-Digital PLL for Frequency Synthesis

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    abstract: Phase locked loops are an integral part of any electronic system that requires a clock signal and find use in a broad range of applications such as clock and data recovery circuits for high speed serial I/O and frequency synthesizers for RF transceivers and ADCs. Traditionally, PLLs have been primarily analog in nature and since the development of the charge pump PLL, they have almost exclusively been analog. Recently, however, much research has been focused on ADPLLs because of their scalability, flexibility and higher noise immunity. This research investigates some of the latest all-digital PLL architectures and discusses the qualities and tradeoffs of each. A highly flexible and scalable all-digital PLL based frequency synthesizer is implemented in 180 nm CMOS process. This implementation makes use of a binary phase detector, also commonly called a bang-bang phase detector, which has potential of use in high-speed, sub-micron processes due to the simplicity of the phase detector which can be implemented with a simple D flip flop. Due to the nonlinearity introduced by the phase detector, there are certain performance limitations. This architecture incorporates a separate frequency control loop which can alleviate some of these limitations, such as lock range and acquisition time.Dissertation/ThesisM.S. Electrical Engineering 201

    Design of CMOS integrated frequency synthesizers for ultra-wideband wireless communications systems

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    Ultraยฌwide band (UWB) system is a breakthrough in wireless communication, as it provides data rate one order higher than existing ones. This dissertation focuses on the design of CMOS integrated frequency synthesizer and its building blocks used in UWB system. A mixerยฌbased frequency synthesizer architecture is proposed to satisfy the agile frequency hopping requirement, which is no more than 9.5 ns, three orders faster than conventional phaseยฌlocked loop (PLL)ยฌbased synthesizers. Harmonic cancelaยฌtion technique is extended and applied to suppress the undesired harmonic mixing components. Simulation shows that sidebands at 2.4 GHz and 5 GHz are below 36 dBc from carrier. The frequency synthesizer contains a novel quadrature VCO based on the capacitive source degeneration structure. The QVCO tackles the jeopardous ambiguity of the oscillation frequency in conventional QVCOs. Measurement shows that the 5ยฌGHz CSDยฌQVCO in 0.18 ยตm CMOS technology draws 5.2 mA current from a 1.2 V power supply. Its phase noise is ยฌ120 dBc at 3 MHz o๏ฌ€set. Compared with existing phase shift LC QVCOs, the proposed CSDยฌQVCO presents better phase noise and power e๏ฌƒciency. Finally, a novel injection locking frequency divider (ILFD) is presented. Imยฌplemented with three stages in 0.18 ยตm CMOS technology, the ILFD draws 3ยฌmA current from a 1.8ยฌV power supply. It achieves multiple large division ratios as 6, 12, and 18 with all locking ranges greater than 1.7 GHz and injection frequency up to 11 GHz. Compared with other published ILFDs, the proposed ILFD achieves the largest division ratio with satisfactory locking range
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