261 research outputs found

    Photonic integration enabling new multiplexing concepts in optical board-to-board and rack-to-rack interconnects

    Get PDF
    New broadband applications are causing the datacenters to proliferate, raising the bar for higher interconnection speeds. So far, optical board-to-board and rack-to-rack interconnects relied primarily on low-cost commodity optical components assembled in a single package. Although this concept proved successful in the first generations of optical-interconnect modules, scalability is a daunting issue as signaling rates extend beyond 25 Gb/s. In this paper we present our work towards the development of two technology platforms for migration beyond Infiniband enhanced data rate (EDR), introducing new concepts in board-to-board and rack-to-rack interconnects. The first platform is developed in the framework of MIRAGE European project and relies on proven VCSEL technology, exploiting the inherent cost, yield, reliability and power consumption advantages of VCSELs. Wavelength multiplexing, PAM-4 modulation and multi-core fiber (MCF) multiplexing are introduced by combining VCSELs with integrated Si and glass photonics as well as BiCMOS electronics. An in-plane MCF-to-SOI interface is demonstrated, allowing coupling from the MCF cores to 340x400 nm Si waveguides. Development of a low-power VCSEL driver with integrated feed-forward equalizer is reported, allowing PAM-4 modulation of a bandwidth-limited VCSEL beyond 25 Gbaud. The second platform, developed within the frames of the European project PHOXTROT, considers the use of modulation formats of increased complexity in the context of optical interconnects. Powered by the evolution of DSP technology and towards an integration path between inter and intra datacenter traffic, this platform investigates optical interconnection system concepts capable to support 16QAM 40GBd data traffic, exploiting the advancements of silicon and polymer technologies

    ์ฐจ์„ธ๋Œ€ ์ž๋™์ฐจ์šฉ ์นด๋ฉ”๋ผ ๋ฐ์ดํ„ฐ ํ†ต์‹ ์„ ์œ„ํ•œ ๋น„๋Œ€์นญ ๋™์‹œ ์–‘๋ฐฉํ–ฅ ์†ก์ˆ˜์‹ ๊ธฐ์˜ ์„ค๊ณ„

    Get PDF
    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2022.2. ์ •๋•๊ท .๋ณธ ํ•™์œ„ ๋…ผ๋ฌธ์—์„œ๋Š” ์ฐจ์„ธ๋Œ€ ์ž๋™์ฐจ์šฉ ์นด๋ฉ”๋ผ ๋งํฌ๋ฅผ ์œ„ํ•ด ๋†’์€ ์†๋„์˜ 4๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์‹ ํ˜ธ์™€ ๋‚ฎ์€ ์†๋„์˜ 2๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์‹ ํ˜ธ๋ฅผ ํ†ต์‹ ํ•˜๋Š” ๋น„๋Œ€์นญ ๋™์‹œ ์–‘๋ฐฉํ–ฅ ์†ก์ˆ˜์‹ ๊ธฐ์˜ ์„ค๊ณ„ ๊ธฐ์ˆ ์— ๋Œ€ํ•ด ์ œ์•ˆํ•˜๊ณ  ๊ฒ€์ฆ๋˜์—ˆ๋‹ค. ์ฒซ๋ฒˆ์งธ ํ”„๋กœํ† ํƒ€์ž… ์„ค๊ณ„์—์„œ๋Š”, 10B6Q ์ง๋ฅ˜ ๋ฐธ๋Ÿฐ์Šค ์ฝ”๋“œ๋ฅผ ํƒ‘์žฌํ•œ 4๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์†ก์‹ ๊ธฐ์™€ ๊ณ ์ •๋œ ๋ฐ์ดํ„ฐ์™€ ์ฐธ์กฐ ๋ ˆ๋ฒจ์„ ๊ฐ€์ง€๋Š” 4๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์ ์‘ํ˜• ์ˆ˜์‹ ๊ธฐ์— ๋Œ€ํ•œ ๋‚ด์šฉ์ด ๊ธฐ์ˆ ๋˜์—ˆ๋‹ค. 4๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์†ก์‹ ๊ธฐ์—์„œ๋Š” ๊ต๋ฅ˜ ์—ฐ๊ฒฐ ๋งํฌ ์‹œ์Šคํ…œ์— ๋Œ€์‘ํ•˜๊ธฐ ์œ„ํ•œ ๋ฉด์  ๋ฐ ์ „๋ ฅ ํšจ์œจ์„ฑ์ด ์ข‹์€ 10B6Q ์ฝ”๋“œ๊ฐ€ ์ œ์•ˆ๋˜์—ˆ๋‹ค. ์ด ์ฝ”๋“œ๋Š” ์ง๋ฅ˜ ๋ฐธ๋Ÿฐ์Šค๋ฅผ ๋งž์ถ”๊ณ  ์—ฐ์†์ ์œผ๋กœ ๊ฐ™์€ ์‹ฌ๋ณผ์„ ๊ฐ€์ง€๋Š” ๊ธธ์ด๋ฅผ 6๊ฐœ๋กœ ์ œํ•œ ์‹œํ‚จ๋‹ค. ๋น„๋ก ์—ฌ๊ธฐ์„œ๋Š” ์ž…๋ ฅ ๋ฐ์ดํ„ฐ ๊ธธ์ด 10๋น„ํŠธ๋ฅผ ์‚ฌ์šฉํ•˜์˜€์ง€๋งŒ, ์ œ์•ˆ๋œ ๊ธฐ์ˆ ์€ ์นด๋ฉ”๋ผ์˜ ๋‹ค์–‘ํ•œ ๋ฐ์ดํ„ฐ ํƒ€์ž…์— ๋Œ€์‘ํ•  ์ˆ˜ ์žˆ๋„๋ก ์ž…๋ ฅ ๋ฐ์ดํ„ฐ ๊ธธ์ด์— ๋Œ€ํ•œ ํ™•์žฅ์„ฑ์„ ๊ฐ€์ง„๋‹ค. ๋ฐ˜๋ฉด, 4๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์ ์‘ํ˜• ์ˆ˜์‹ ๊ธฐ์—์„œ๋Š”, ์ƒ˜ํ”Œ๋Ÿฌ์˜ ์˜ต์…‹์„ ์ตœ์ ์œผ๋กœ ์ œ๊ฑฐํ•˜์—ฌ ๋” ๋‚ฎ์€ ๋น„ํŠธ์—๋Ÿฌ์œจ์„ ์–ป๊ธฐ ์œ„ํ•ด์„œ, ๊ธฐ์กด์˜ ๋ฐ์ดํ„ฐ ๋ฐ ์ฐธ์กฐ ๋ ˆ๋ฒจ์„ ์กฐ์ ˆํ•˜๋Š” ๋Œ€์‹ , ์ด ๋ ˆ๋ฒจ๋“ค์€ ๊ณ ์ •์‹œํ‚ค๊ณ  ๊ฐ€๋ณ€ ๊ฒŒ์ธ ์ฆํญ๊ธฐ๋ฅผ ์ ์‘ํ˜•์œผ๋กœ ์กฐ์ ˆํ•˜๋„๋ก ํ•˜์˜€๋‹ค. ์ƒ๊ธฐ 10B6Q ์ฝ”๋“œ ๋ฐ ๊ณ ์ • ๋ฐ์ดํ„ฐ ๋ฐ ์ฐธ์กฐ๋ ˆ๋ฒจ ๊ธฐ์ˆ ์„ ๊ฐ€์ง„ ํ”„๋กœํ† ํƒ€์ž… ์นฉ๋“ค์€ 40 ๋‚˜๋…ธ๋ฏธํ„ฐ ์ƒํ˜ธ๋ณด์™„ํ˜• ๋ฉ”ํƒˆ ์‚ฐํ™” ๋ฐ˜๋„์ฒด ๊ณต์ •์œผ๋กœ ์ œ์ž‘๋˜์—ˆ๊ณ  ์นฉ ์˜จ ๋ณด๋“œ ํ˜•ํƒœ๋กœ ํ‰๊ฐ€๋˜์—ˆ๋‹ค. 10B6Q ์ฝ”๋“œ๋Š” ํ•ฉ์„ฑ ๊ฒŒ์ดํŠธ ์ˆซ์ž๋Š” 645๊ฐœ์™€ ํ•จ๊ป˜ ๋‹จ 0.0009 mm2 ์˜ ๋ฉด์  ๋งŒ์„ ์ฐจ์ง€ํ•œ๋‹ค. ๋˜ํ•œ, 667 MHz ๋™์ž‘ ์ฃผํŒŒ์ˆ˜์—์„œ ๋‹จ 0.23 mW ์˜ ์ „๋ ฅ์„ ์†Œ๋ชจํ•œ๋‹ค. 10B6Q ์ฝ”๋“œ๋ฅผ ํƒ‘์žฌํ•œ ์†ก์‹ ๊ธฐ์—์„œ 8-Gb/s 4๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์‹ ํ˜ธ๋ฅผ ๊ณ ์ • ๋ฐ์ดํ„ฐ ๋ฐ ์ฐธ์กฐ ๋ ˆ๋ฒจ์„ ๊ฐ€์ง€๋Š” ์ ์‘ํ˜• ์ˆ˜์‹ ๊ธฐ๋กœ 12-m ์ผ€์ด๋ธ” (22-dB ์ฑ„๋„ ๋กœ์Šค) ์„ ํ†ตํ•ด์„œ ๋ณด๋‚ธ ๊ฒฐ๊ณผ ์ตœ์†Œ ๋น„ํŠธ ์—๋Ÿฌ์œจ 108 ์„ ๋‹ฌ์„ฑํ•˜์˜€๊ณ , ๋น„ํŠธ ์—๋Ÿฌ์œจ 105 ์—์„œ๋Š” ์•„์ด ๋งˆ์ง„์ด 0.15 UI x 50 mV ๋ณด๋‹ค ํฌ๊ฒŒ ์ธก์ •๋˜์—ˆ๋‹ค. ์†ก์ˆ˜์‹ ๊ธฐ๋ฅผ ํ•ฉ์นœ ์ „๋ ฅ ์†Œ๋ชจ๋Š” 65.2 mW (PLL ์ œ์™ธ) ์ด๊ณ , ์„ฑ๊ณผ์˜ ๋Œ€ํ‘œ์ˆ˜์น˜๋Š” 0.37 pJ/b/dB ๋ฅผ ๋ณด์—ฌ์ฃผ์—ˆ๋‹ค. ์ฒซ๋ฒˆ์งธ ํ”„๋กœํ† ํƒ€์ž… ์„ค๊ณ„์„ ํฌํ•จํ•˜์—ฌ ๊ฐœ์„ ๋œ ๋‘๋ฒˆ์งธ ํ”„๋กœํ† ํƒ€์ž… ์„ค๊ณ„์—์„œ๋Š”, 12-Gb/s 4๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์ •๋ฐฉํ–ฅ ์ฑ„๋„ ์‹ ํ˜ธ์™€ 125-Mb/s 2๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์—ญ๋ฐฉํ–ฅ ์ฑ„๋„ ์‹ ํ˜ธ๋ฅผ ํƒ‘์žฌํ•œ ๋น„๋Œ€์นญ ๋™์‹œ ์–‘๋ฐฉํ–ฅ ์†ก์ˆ˜์‹ ๊ธฐ์— ๋Œ€ํ•ด ๊ธฐ์ˆ ๋˜๊ณ  ๊ฒ€์ฆ๋˜์—ˆ๋‹ค. ์ œ์•ˆ๋œ ๋„“์€ ์„ ํ˜• ๋ฒ”์œ„๋ฅผ ๊ฐ€์ง€๋Š” ํ•˜์ด๋ธŒ๋ฆฌ๋“œ๋Š” gmC ์ €๋Œ€์—ญ ํ†ต๊ณผ ํ•„ํ„ฐ์™€ ์—์ฝ” ์ œ๊ฑฐ๊ธฐ์™€ ํ•จ๊ป˜ ์•„์›ƒ๋ฐ”์šด๋“œ ์‹ ํ˜ธ๋ฅผ 24 dB ์ด์ƒ ํšจ์œจ์ ์œผ๋กœ ๊ฐ์†Œ์‹œ์ผฐ๋‹ค. ๋˜ํ•œ, ๋„“์€ ์„ ํ˜• ๋ฒ”์œ„๋ฅผ ๊ฐ€์ง€๋Š” ํ•˜์ด๋ธŒ๋ฆฌ๋“œ์™€ ํ•จ๊ป˜ ๊ฒŒ์ธ ๊ฐ์†Œ๊ธฐ๋ฅผ ํ˜•์„ฑํ•˜๊ฒŒ ๋˜๋Š” ์„ ํ˜• ๋ฒ”์œ„ ์ฆํญ๊ธฐ๋ฅผ ํ†ตํ•ด 4๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์‹ ํ˜ธ์˜ ์„ ํ˜•์„ฑ๊ณผ ์ง„ํญ์˜ ํŠธ๋ ˆ์ด๋“œ ์˜คํ”„ ๊ด€๊ณ„๋ฅผ ๊นจ๋Š” ๊ฒƒ์ด ๊ฐ€๋Šฅํ•˜์˜€๋‹ค. ๋™์‹œ ์–‘๋ฐฉํ–ฅ ์†ก์ˆ˜์‹ ๊ธฐ ์นฉ์€ 40 ๋‚˜๋…ธ๋ฏธํ„ฐ ์ƒํ˜ธ๋ณด์™„ํ˜• ๋ฉ”ํƒˆ ์‚ฐํ™” ๋ฐ˜๋„์ฒด ๊ณต์ •์œผ๋กœ ์ œ์ž‘๋˜์—ˆ๋‹ค. ์ƒ๊ธฐ ์„ค๊ณ„ ๊ธฐ์ˆ ๋“ค์„ ์ด์šฉํ•˜์—ฌ, 4๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ๋ฐ 2๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์†ก์ˆ˜์‹ ๊ธฐ ๋ชจ๋‘ 5m ์ฑ„๋„ (์ฑ„๋„ ๋กœ์Šค 15.9 dB) ์—์„œ 1E-12 ๋ณด๋‹ค ๋‚ฎ์€ ๋น„ํŠธ ์—๋Ÿฌ์œจ์„ ๋‹ฌ์„ฑํ•˜์˜€๊ณ , ์ด 78.4 mW ์˜ ์ „๋ ฅ ์†Œ๋ชจ๋ฅผ ๊ธฐ๋กํ•˜์˜€๋‹ค. ์ข…ํ•ฉ์ ์ธ ์†ก์ˆ˜์‹ ๊ธฐ๋Š” ์„ฑ๊ณผ ๋Œ€ํ‘œ์ง€ํ‘œ๋กœ 0.41 pJ/b/dB ์™€ ํ•จ๊ป˜ ๋™์‹œ ์–‘๋ฐฉํ–ฅ ํ†ต์‹  ์•„๋ž˜์—์„œ 4๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์‹ ํ˜ธ ๋ฐ 2๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ์‹ ํ˜ธ ๊ฐ๊ฐ์—์„œ ์•„์ด ๋งˆ์ง„ 0.15 UI ์™€ 0.57 UI ๋ฅผ ๋‹ฌ์„ฑํ•˜์˜€๋‹ค. ์ด ์ˆ˜์น˜๋Š” ์„ฑ๊ณผ ๋Œ€ํ‘œ์ง€ํ‘œ 0.5 ์ดํ•˜๋ฅผ ๊ฐ€์ง€๋Š” ๊ธฐ์กด ๋™์‹œ ์–‘๋ฐฉํ–ฅ ์†ก์ˆ˜์‹ ๊ธฐ์™€์˜ ๋น„๊ต์—์„œ ์ตœ๊ณ ์˜ ์•„์ด ๋งˆ์ง„์„ ๊ธฐ๋กํ•˜์˜€๋‹ค.In this dissertation, design techniques of a highly asymmetric simultaneous bidirectional (SB) transceivers with high-speed PAM-4 and low-speed PAM-2 signals are proposed and demonstrated for the next-generation automotive camera link. In a first prototype design, a PAM-4 transmitter with 10B6Q DC balance code and a PAM-4 adaptive receiver with fixed data and threshold levels (dtLevs) are presented. In PAM-4 transmitter, an area- and power-efficient 10B6Q code for an AC coupled link system that guarantees DC balance and limited run length of six is proposed. Although the input data width of 10 bits is used here, the proposed scheme has an extensibility for the input data width to cover various data types of the camera. On the other hand, in the PAM-4 adaptive receiver, to optimally cancel the sampler offset for a lower BER, instead of adjusting dtLevs, the gain of a programmable gain amplifier is adjusted adaptively under fixed dtLevs. The prototype chips including above proposed 10B6Q code and fixed dtLevs are fabricated in 40-nm CMOS technology and tested in chip-on-board assembly. The 10B6Q code only occupies an active area of 0.0009 mm2 with a synthesized gate count of 645. It also consumes 0.23 mW at the operating clock frequency of 667 MHz. The transmitter with 10B6Q code delivers 8-Gb/s PAM-4 signal to the adaptive receiver using fixed dtLevs through a lossy 12-m cable (22-dB channel loss) with a BER of 1E-8, and the eye margin larger than 0.15 UI x 50 mV is measured for a BER of 1E-5. The proto-type chips consume 65.2 mW (excluding PLL), exhibiting an FoM of 0.37 pJ/b/dB. In a second prototype design advanced from the first prototypes, An asymmetric SB transceivers incorporating a 12-Gb/s PAM-4 forward channel and a 125-Mb/s PAM-2 back channel are presented and demonstrated. The proposed wide linear range (WLR) hybrid combined with a gmC low-pass filter and an echo canceller effectively suppresses the outbound signals by more than 24dB. In addition, linear range enhancer which forms a gain attenuator with WLR hybrid breaks the trade-off between the linearity and the amplitude of the PAM-4 signal. The SB transceiver chips are separately fabricated in 40-nm CMOS technology. Using above design techniques, both PAM-4 and PAM-2 SB transceivers achieve BER less than 1E-12 over a 5-m channel (15.9 dB channel loss), consuming 78.4 mW. The overall transceivers achieve an FoM of 0.41 pJ/b/dB and eye margin (at BER of 1E-12) of 0.15 UI and 0.57 UI for the forward PAM-4 and back PAM-2 signals, respectively, under SB communication. This is the best eye margin compared to the prior art SB transceivers with an FoM less than 0.5.CHAPTER 1 INTRODUCTION 1 1.1 MOTIVATION 1 1.2 DISSERTATION ORGANIZATION 4 CHAPTER 2 BACKGROUND ON AUTOMOTIVE CAMERA LINK 6 2.1 OVERVIEW 6 2.2 SYSTEM REQUIREMENTS 10 2.2.1 CHANNEL 10 2.2.2 POWER OVER DIFFERENTIAL LINE (PODL) 12 2.2.3 AC COUPLING AND DC BALANCE CODE 15 2.2.4 SIMULTANEOUS BIDIRECTIONAL COMMUNICATION 18 2.2.4.1 HYBRID 18 2.2.4.2 ECHO CANCELLER 20 2.2.5 ADAPTIVE RECEIVE EQUALIZATION 22 CHAPTER 3 AREA AND POWER EFFICIENT 10B6Q ENCODER FOR DC BALANCE 25 3.1 INTRODUCTION 25 3.2 PRIOR WORKS 28 3.3 PROPOSED AREA- AND POWER-EFFICIENT 10B6Q PAM-4 CODER 30 3.4 DESIGN OF THE 10B6Q CODE 33 3.4.1 PAM-4 DC BALANCE 35 3.4.2 PAM-4 TRANSITION DENSITY 35 3.4.3 10B6Q DECODER 37 3.5 IMPLEMENTATION AND MEASUREMENT RESULTS 40 CHAPTER 4 PAM-4 TRANSMITTER AND ADAPTIVE RECEIVER WITH FIXED DATA AND THRESHOLD LEVELS 45 4.1 INTRODUCTION 45 4.2 PRIOR WORKS 47 4.3 ARCHITECTURE AND IMPLEMENTATION 49 4.2.1 PAM-4 TRANSMITTER 49 4.2.2 PAM-4 ADAPTIVE RECEIVER 52 4.3 MEASUREMENT RESULTS 62 CHAPTER 5 ASYMMETRIC SIMULTANEOUS BIDIRECTIONAL TRANSCEIVERS USING WIDE LINEAR RANGE HYBRID 68 5.1 INTRODUCTION 68 5.2 PRIOR WORKS 70 5.3 WIDE LINEAR RANGE (WLR) HYBRID 75 5.3 IMPLEMENTATION 78 5.3.1 SERIALIZER (SER) DESIGN 78 5.3.2 DESERIALIZER (DES) DESIGN 79 5.4 HALF CIRCUIT ANALYSIS OF WLR HYBRID AND LRE 82 5.5 MEASUREMENT RESULTS 88 CHAPTER 6 CONCLUSION 97 BIBLIOGRAPHY 99 ์ดˆ ๋ก 106๋ฐ•

    A 160Gb/s (4x40) WDM O-band Tx subassembly using a 4-ch array of silicon rings co-packaged with a SiGe BiCMOS IC driver

    Get PDF
    We present a 400 (8ร—50) Gb/s-capable RM-based Si-photonic WDM O-band TxRx with 1.17nm channel spacing for high-speed optical interconnects and demonstrate successful 50Gb/s-NRZ TxRx operation achieving a ~4.5dB Tx extinction ratio under 2.15Vpp drive

    Integrated Circuit Design for Hybrid Optoelectronic Interconnects

    Get PDF
    This dissertation focuses on high-speed circuit design for the integration of hybrid optoelectronic interconnects. It bridges the gap between electronic circuit design and optical device design by seamlessly incorporating the compact Verilog-A model for optical components into the SPICE-like simulation environment, such as the Cadence design tool. Optical components fabricated in the IME 130nm SOI CMOS process are characterized. Corresponding compact Verilog-A models for Mach-Zehnder modulator (MZM) device are developed. With this approach, electro-optical co-design and hybrid simulation are made possible. The developed optical models are used for analyzing the system-level specifications of an MZM based optoelectronic transceiver link. Link power budgets for NRZ, PAM-4 and PAM-8 signaling modulations are simulated at system-level. The optimal transmitter extinction ratio (ER) is derived based on the required receiver\u27s minimum optical modulation amplitude (OMA). A limiting receiver is fabricated in the IBM 130 nm CMOS process. By side- by-side wire-bonding to a commercial high-speed InGaAs/InP PIN photodiode, we demonstrate that the hybrid optoelectronic limiting receiver can achieve the bit error rate (BER) of 10-12 with a -6.7 dBm sensitivity at 4 Gb/s. A full-rate, 4-channel 29-1 length parallel PRBS is fabricated in the IBM 130 nm SiGe BiCMOS process. Together with a 10 GHz phase locked loop (PLL) designed from system architecture to transistor level design, the PRBS is demonstrated operating at more than 10 Gb/s. Lessons learned from high-speed PCB design, dealing with signal integrity issue regarding to the PCB transmission line are summarized

    Silicon photonic modulators for PAM transmissions

    Get PDF
    High-speed optical interconnects are crucial for both data centers and high performance computing systems. High power consumption and limited device bandwidth have hindered the move to higher optical transmission speeds. Integrated optical transceivers in silicon photonics (SiP) using pulse-amplitude modulation (PAM) are a promising solution to increase data rates. In this paper, we review recent progress in SiP for PAM transmissions. We focus on materials and technologies available CMOS-compatible photonics processes. Performance metrics of SiP modulators and crucial considerations for high-speed PAM transmissions are discussed. Various driving strategies to achieve optical PAM signals are presented. Some of the state-of-the-art SiP PAM modulators and integrated transmitters are reviewed

    Transmetteurs photoniques sur silicium pour les transmissions optiques ร  grande capacitรฉ

    Get PDF
    Les applications exigeant des trรจs nombreuses donnรฉes (mรฉdias sociaux, diffusion vidรฉo en continu, mรฉgadonnรฉes, etc.) se dรฉveloppent ร  un rythme rapide, ce qui nรฉcessite de plus en plus de liaisons optiques ultra-rapides. Ceci implique le dรฉveloppment des transmetteurs optiques intรฉgrรฉs et ร  bas coรปt et plus particulirement en photonique sur silicium en raison de ses avantages par rapport aux autres technologies (LiNbO3 et InP), tel que la compatibilitรฉ avec le procรฉdรฉ de fabrication CMOS. Les modulateurs optoรฉlectronique sont un รฉlรฉment essentiel dans la communication op-tique. Beaucoup de travaux de recherche sont consacrรฉes au dรฉveloppement de dispositifs optiques haut dรฉbit efficaces. Cependant, la conception de modulateurs en photonique sur sili-cium (SiP) haut dรฉbit est diffcile, principalement en raison de l'absence d'effet รฉlectro-optique intrinsรจque dans le silicium. De nouvelles approches et de architectures plus performances doivent รชtre dรฉveloppรฉes afin de satisfaire aux critรจres rรฉliรฉs au systรจme d'une liaison optique aux paramรจtres de conception au niveau du dispositif integrรฉ. En outre, la co-conception de circuits integrรฉs photoniques sur silicium et CMOS est cruciale pour atteindre tout le potentiel de la technologie de photonique sur silicium. Ainsi cette thรจse aborde les dรฉfits susmentionnรฉs. Dans notre premiรจre contribution, nous prรฉesentons pour la premiรจre fois un รฉmetteur phononique sur silicium PAM-4 sans utiliser un convertisseur numรฉrique analog (DAC)qui comprend un modulateur Mach Zehnder ร  รฉlectrodes segmentรฉes SiP (LES-MZM) implรฉmentรฉ dans un procรฉdรฉ photonique sur silicium gรฉnรฉrique avec jonction PN latรฉrale et son conducteur CMOS intรฉgrรฉ. Des dรฉbits allant jusqu'ร  38 Gb/s/chnnel sont obtenus sans utili-ser un convertisseur numรฉrique-analogique externe. Nous prรฉsentons รฉgalement une nouvelle procรฉdure de gรฉnรฉration de dรฉlai dans le excitateur de MOS complรฉmentaire. Un effet, un dรฉlai robuste aussi petit que 7 ps est gรฉnรฉrรฉ entre les canaux de conduite. Dans notre deuxiรจme contribution, nous prรฉsentons pour la premiรจre fois un nouveau fac-teur de mรฉrite (FDM) pour les modulateurs SiP qui inclut non seulement la perte optique et l'efficacitรฉ (comme les FDMs prรฉcรฉdents), mais aussi la bande passante รฉlectro-optique du modulateur SiP (BWEO). Ce nouveau FDM peut faire correspondre les paramรจtres de conception physique du modulateur SiP ร  ses critรจres de performance au niveau du systรจme, facilitant ร  la fois la conception du dispositif optique et l'optimisation du systรจme. Pour la premiรจre fois nous dรฉfinissons et utilisons la pรฉnalitรฉ de puissance du modulateur (MPP) induite par le modulateur SiP pour รฉtudier la dรฉgradation des performances au niveau du systรจme induite par le modulateur SiP dans une communication ร  base de modulation d'amplitude d'impulsion optique. Nous avons dรฉveloppรฉ l'รฉquation pour MPP qui inclut les facteurs de limitation du modulateur (perte optique, taux d'extinction limitรฉ et limitation de la bande passante รฉlectro-optique). Enfin, dans notre troisiรจme contribution, une nouvelle mรฉthodologie de conception pour les modulateurs en SiP intรฉgrรฉ ร  haute dรฉbit est prรฉsentรฉe. La nouvelle approche est basรฉe sur la minimisation de la MPP SiP en optimisant l'architecture du modulateur et le point de fonctionnement. Pour ce processus, une conception en longueur unitaire du modulateur Mach Zehnder (MZM) peut รชtre optimisรฉe en suivant les spรฉcifications du procรฉdรฉ de fabrication et les rรจgles de conception. Cependant, la longueur et la tension de biais du d'รฉphaseur doivent รชtre optimisรฉes ensemble (par exemple selon vitesse de transmission et format de modulation). Pour vรฉrifier l'approche d'optimisation proposรฉe expรฉrimentale mont, a conรงu un modulateur photonique sur silicium en phase / quadrature de phase (IQ) ciblant le format de modulation 16-QAM ร  60 Gigabaud. Les rรฉsultats expรฉrimentaux prouvent la fiabilitรฉ de la mรฉthodologie proposรฉe. D'ailleurs, nous avons augmentรฉ la vitesse de transmission jusqu'ร  70 Gigabaud pour tester la limite de dรฉbit au systรจme. Une transmission de donnรฉes dos ร  dos avec des dรฉbits binaires de plus de 233 Gigabit/s/channel est observรฉe. Cette mรฉthodologie de conception ouvre ainsi la voie ร  la conception de la prochaine gรฉnรฉration d'รฉmetteurs intรฉgrรฉs ร  double polarisation 400+ Gigabit/s/channel.Data-hungry applications (social media, video streaming, big data, etc.) are expanding at a fast pace, growing demand for ultra-fast optical links. This driving force reveals need for low-cost, integrated optical transmitters and pushes research in silicon photonics because of its advantages over other platforms (i.e. LiNbO3 and InP), such as compatibility with CMOS fabrication processes, the ability of on-chip polarization manipulation, and cost effciency. Electro-optic modulators are an essential component of optical communication links and immense research is dedicated to developing effcient high-bitrate devices. However, the design of high-capacity Silicon Photonics (SiP) transmitters is challenging, mainly due to lack of inherent electro-optic effect in silicon. New design methodologies and performance merits have to be developed in order to map the system-level criteria of an optical link to the design parameters in device-level. In addition, co-design of silicon photonics and CMOS integrated circuits is crucial to reveal the full potential of silicon photonics. This thesis addresses the aforementioned challenges. In our frst contribution, for the frst time we present a DAC-less PAM-4 silicon photonic transmitter that includes a SiP lumped-element segmented-electrode Mach Zehnder modula-tor (LES-MZM) implemented in a generic silicon photonic process with lateral p-n junction and its co-designed CMOS driver. Using post processing, bitrates up to 38 Gb/s/channel are achieved without using an external digital to analog converter. We also presents a novel delay generation procedure in the CMOS driver. A robust delay as small as 7 ps is generated between the driving channels. In our second contribution, for the frst time we present a new figure of merit (FOM) for SiP modulators that includes not only the optical loss and effciency (like the prior FOMs), but also the SiP modulator electro-optic bandwidth ( BWEO). This new FOM can map SiP modulator physical design parameters to its system-level performance criteria, facilitating both device design and system optimization. For the frst time we define and employ the modulator power penalty (MPP) induced by the SiP modulator to study the system level performance degradation induced by SiP modulator in an optical pulse amplitude modulation link. We develope a closed-form equation for MPP that includes the SiP modulator limiting factors (optical loss, limited extinction ratio and electro-optic bandwidth limitation). Finally in our third contribution, we present a novel design methodology for integrated high capacity SiP modulators. The new approach is based on minimizing the power penalty of a SiP modulator (MPP) by optimizing modulator design and bias point. For the given process, a unit-length design of Mach Zehnder modulator (MZM) can be optimized following the process specifications and design rules. However, the length and the bias voltage of the phase shifter must be optimized together in a system context (e.g., baud rate and modulation format). Moreover, to verify the proposed optimization approach in experiment, we design an in-phase/quadrature-phase (IQ) silicon photonic modulator targeting 16-QAM modulation format at 60 Gbaud. Experimental results proves the reliability of our proposed methodology. We further push the baud rate up to 70 Gbaud to examine the capacity boundary of the device. Back to back data transmission with bitrates more than 233 Gb/s/channel are captured. This design methodology paves the way for designing the next generation of integrated dual- polarization 400+ Gb/s/channel transmitters

    ๋Œ€์—ญํญ ์ฆ๋Œ€ ๊ธฐ์ˆ ์„ ์ด์šฉํ•œ ์ „๋ ฅ ํšจ์œจ์  ๊ณ ์† ์†ก์‹  ์‹œ์Šคํ…œ ์„ค๊ณ„

    Get PDF
    ํ•™์œ„๋…ผ๋ฌธ(๋ฐ•์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2022.2. ์ •๋•๊ท .The high-speed interconnect at the datacenter is being more crucial as 400 Gb Ethernet standards are developed. At the high data rate, channel loss re-quires bandwidth extension techniques for transmitters, even for short-reach channels. On the other hand, as the importance of east-to-west connection is rising, the data center architectures are switching to spine-leaf from traditional ones. In this trend, the number of short-reach optical interconnect is expected to be dominant. The vertical-cavity surface-emitting laser (VCSEL) is a com-monly used optical modulator for short-reach interconnect. However, since VCSEL has low bandwidth and nonlinearity, the optical transmitter also needs bandwidth-increasing techniques. Additionally, the power consumption of data centers reaches a point of concern to affect climate change. Therefore, this the-sis focuses on high-speed, power-efficient transmitters for data center applica-tions. Before the presenting circuit design, bandwidth extension techniques such as fractionally-spaced feed-forward equalizer (FFE), on-chip transmission line, inductive peaking, and T-coil are mathematically analyzed for their effec-tiveness. For the first chip, a power and area-efficient pulse-amplitude modulation 4 (PAM-4) transmitter using 3-tap FFE based on a slow-wave transmission line is presented. A passive delay line is adopted for generating an equalizer tap to overcome the high clocking power consumption. The transmission line achieves a high slow-wave factor of 15 with double floating metal shields around the differential coplanar waveguide. The transmitter includes 4:1 multi-plexers (MUXs) and a quadrature clock generator for high-speed data genera-tion in a quarter-rate system. The 4:1 MUX utilizes a 2-UI pulse generator, and the input configuration is determined by qualitative analysis. The chip is fabri-cated in 65 nm CMOS technology and occupies an area of 0.151 mm2. The proposed transmitter system exhibits an energy efficiency of 3.03 pJ/b at the data rate of 48 Gb/s with PAM-4 signaling. The second chip presents a power-efficient PAM-4 VCSEL transmitter using 3-tap FFE and negative-k T-coil. The phase interpolators (PIs) generate frac-tionally-spaced FFE tap and correct quadrature phase error. The PAM-4 com-bining 8:1 MUX is proposed rather than combining at output driver with double 4:1 MUXs to reduce serializing power consumption. T-coils at the internal and output node increase the bandwidth and remove inter-symbol interference (ISI). The negative-k T-coil at the output network increases the bandwidth 1.61 times than without T-coil. The VCSEL driver is placed on the high VSS domain for anode driving and power reduction. The chip is fabricated in 40 nm CMOS technology. The proposed VCSEL transmitter operates up to 48 Gb/s NRZ and 64 Gb/s PAM-4 with the power efficiency of 3.03 pJ/b and 2.09 pJ/b, respec-tively.400Gb ์ด๋”๋„ท ํ‘œ์ค€์ด ๊ฐœ๋ฐœ๋จ์— ๋”ฐ๋ผ ๋ฐ์ดํ„ฐ ์„ผํ„ฐ์˜ ๊ณ ์† ์ƒํ˜ธ ์—ฐ๊ฒฐ์ด ๋”์šฑ ์ค‘์š”ํ•ด์ง€๊ณ  ์žˆ๋‹ค. ๋†’์€ ๋ฐ์ดํ„ฐ ์†๋„์—์„œ์˜ ์ฑ„๋„ ์†์‹ค์— ์˜ํ•ด ๋‹จ๊ฑฐ๋ฆฌ ์ฑ„๋„์˜ ๊ฒฝ์šฐ์—๋„ ์†ก์‹ ๊ธฐ์— ๋Œ€ํ•œ ๋Œ€์—ญํญ ํ™•์žฅ ๊ธฐ์ˆ ์ด ํ•„์š”ํ•˜๋‹ค. ํ•œํŽธ, ๋ฐ์ดํ„ฐ ์„ผํ„ฐ ๋‚ด ๋™-์„œ ์—ฐ๊ฒฐ์˜ ์ค‘์š”์„ฑ์ด ๋†’์•„์ง€๋ฉด์„œ ๋ฐ์ดํ„ฐ ์„ผํ„ฐ ์•„ํ‚คํ…์ฒ˜๊ฐ€ ๊ธฐ์กด์˜ ์•„ํ‚คํ…์ฒ˜์—์„œ ์ŠคํŒŒ์ธ-๋ฆฌํ”„๋กœ ์ „ํ™˜๋˜๊ณ  ์žˆ๋‹ค. ์ด๋Ÿฌํ•œ ์ถ”์„ธ์—์„œ ๋‹จ๊ฑฐ๋ฆฌ ๊ด‘ํ•™ ์ธํ„ฐ์ปค๋„ฅํŠธ์˜ ์ˆ˜๊ฐ€ ์ ์ฐจ ์šฐ์„ธํ•ด์งˆ ๊ฒƒ์œผ๋กœ ์˜ˆ์ƒ๋œ๋‹ค. ์ˆ˜์ง ์บ๋น„ํ‹ฐ ํ‘œ๋ฉด ๋ฐฉ์ถœ ๋ ˆ์ด์ €(VCSEL)๋Š” ์ผ๋ฐ˜์ ์œผ๋กœ ๋‹จ๊ฑฐ๋ฆฌ ์ƒํ˜ธ ์—ฐ๊ฒฐ์„ ์œ„ํ•ด ์‚ฌ์šฉ๋˜๋Š” ๊ด‘ํ•™ ๋ชจ๋“ˆ๋ ˆ์ดํ„ฐ์ด๋‹ค. VCSEL์€ ๋‚ฎ์€ ๋Œ€์—ญํญ๊ณผ ๋น„์„ ํ˜•์„ฑ์„ ๊ฐ€์ง€๊ณ  ์žˆ๊ธฐ ๋•Œ๋ฌธ์—, ๊ด‘ ์†ก์‹ ๊ธฐ๋„ ๋Œ€์—ญํญ ์ฆ๊ฐ€ ๊ธฐ์ˆ ์„ ํ•„์š”๋กœ ํ•œ๋‹ค. ๋˜ํ•œ, ๋ฐ์ดํ„ฐ ์„ผํ„ฐ์˜ ์ „๋ ฅ ์†Œ๋น„๋Š” ๊ธฐํ›„ ๋ณ€ํ™”์— ์˜ํ–ฅ์„ ๋ฏธ์น  ์ˆ˜ ์žˆ๋Š” ์šฐ๋ ค ์ง€์ ์— ๋„๋‹ฌํ–ˆ๋‹ค. ๋”ฐ๋ผ์„œ, ๋ณธ ๋…ผ๋ฌธ์€ ๋ฐ์ดํ„ฐ ์„ผํ„ฐ ์‘์šฉ์„ ์œ„ํ•œ ๊ณ ์† ์ „๋ ฅ ํšจ์œจ์ ์ธ ์†ก์‹ ๊ธฐ์— ์ดˆ์ ์„ ๋งž์ถ”๊ณ  ์žˆ๋‹ค. ํšŒ๋กœ ์„ค๊ณ„๋ฅผ ์ œ์‹œํ•˜๊ธฐ ์ „์—, ๋ถ€๋ถ„ ๊ฐ„๊ฒฉ ํ”ผ๋“œ-ํฌ์›Œ๋“œ ์ดํ€„๋ผ์ด์ € (FFE), ์˜จ์นฉ ์ „์†ก์„ ๋กœ, ์ธ๋•ํ„ฐ, T-์ฝ”์ผ๊ณผ ๊ฐ™์€ ๋Œ€์—ญํญ ํ™•์žฅ ๊ธฐ์ˆ ์„ ์ˆ˜ํ•™์ ์œผ๋กœ ๋ถ„์„ํ•œ๋‹ค. ์ฒซ ๋ฒˆ์งธ ์นฉ์€ ์ €์†ํŒŒ ์ „์†ก์„ ๋กœ๋ฅผ ๊ธฐ๋ฐ˜์œผ๋กœ ํ•œ 3-ํƒญ FFE๋ฅผ ์‚ฌ์šฉํ•˜๋Š” ์ „๋ ฅ ๋ฐ ๋ฉด์  ํšจ์œจ์ ์ธ ํŽ„์Šค-์ง„ํญ-๋ณ€์กฐ 4(PAM-4) ์†ก์‹ ๊ธฐ๋ฅผ ์ œ์‹œํ•œ๋‹ค. ๋†’์€ ํด๋Ÿญ ์ „๋ ฅ ์†Œ๋น„๋ฅผ ๊ทน๋ณตํ•˜๊ธฐ ์œ„ํ•ด ์ดํ€„๋ผ์ด์ € ํƒญ ์ƒ์„ฑ์„ ์œ„ํ•ด ์ˆ˜๋™์†Œ์ž ์ง€์—ฐ ๋ผ์ธ์„ ์ฑ„ํƒํ–ˆ๋‹ค. ์ „์†ก ๋ผ์ธ์€ ์ฐจ๋™ ๋™์ผํ‰๋ฉด๋„ํŒŒ๊ด€ ์ฃผ์œ„์— ์ด์ค‘ ํ”Œ๋กœํŒ… ๊ธˆ์† ์ฐจํ๋ฅผ ์‚ฌ์šฉํ•˜์—ฌ 15์˜ ๋†’์€ ์ „๋‹ฌ์†๋„ ๊ฐ์‡ ๋ฅผ ๋‹ฌ์„ฑํ•œ๋‹ค. ์†ก์‹ ๊ธฐ์—๋Š” 4:1 ๋ฉ€ํ‹ฐํ”Œ๋ ‰์„œ(MUX)์™€ 4-์œ„์ƒ ํด๋Ÿญ ์ƒ์„ฑ๊ธฐ๊ฐ€ ํฌํ•จ๋˜์–ด ์žˆ๋‹ค. 4:1 MUX๋Š” 2-UI ํŽ„์Šค ๋ฐœ์ƒ๊ธฐ๋ฅผ ์‚ฌ์šฉํ•˜๋ฉฐ, ์ •์„ฑ ๋ถ„์„์— ์˜ํ•ด ์ž…๋ ฅ ๊ตฌ์„ฑ์ด ๊ฒฐ์ •๋œ๋‹ค. ์ด ์นฉ์€ 65 nm CMOS ๊ธฐ์ˆ ๋กœ ์ œ์ž‘๋˜์—ˆ์œผ๋ฉฐ 0.151 mm2์˜ ๋ฉด์ ์„ ์ฐจ์ง€ํ•œ๋‹ค. ์ œ์•ˆ๋œ ์†ก์‹ ๊ธฐ ์‹œ์Šคํ…œ์€ PAM-4 ์‹ ํ˜ธ์™€ ํ•จ๊ป˜ 48 Gb/s์˜ ๋ฐ์ดํ„ฐ ์†๋„์—์„œ 3.03 pJ/b์˜ ์—๋„ˆ์ง€ ํšจ์œจ์„ ๋ณด์—ฌ์ค€๋‹ค. ๋‘ ๋ฒˆ์งธ ์นฉ์—์„œ๋Š” 3-ํƒญ FFE ๋ฐ ์—ญํšŒ์ „ T-์ฝ”์ผ์„ ์‚ฌ์šฉํ•˜๋Š” ์ „๋ ฅ ํšจ์œจ์ ์ธ PAM-4 VCSEL ์†ก์‹ ๊ธฐ๋ฅผ ์ œ์‹œํ•œ๋‹ค. ์œ„์ƒ ๋ณด๊ฐ„๊ธฐ(PI)๋Š” ๋ถ€๋ถ„ ๊ฐ„๊ฒฉ FFE ํƒญ์„ ์ƒ์„ฑํ•˜๊ณ  4-์œ„์ƒ ํด๋Ÿญ ์˜ค๋ฅ˜๋ฅผ ์ˆ˜์ •ํ•˜๋Š” ๋ฐ ์‚ฌ์šฉ๋œ๋‹ค. ์ง๋ ฌํ™” ์ „๋ ฅ ์†Œ๋น„๋ฅผ ์ค„์ด๊ธฐ ์œ„ํ•ด ์ถœ๋ ฅ ๋“œ๋ผ์ด๋ฒ„์—์„œ MSB์™€ LSB๋ฅผ ๋‘ ๊ฐœ์˜ 4:1 MUX๋ฅผ ํ†ตํ•ด ๊ฒฐํ•ฉํ•˜๋Š” ๋Œ€์‹  8:1 MUX๋ฅผ ํ†ตํ•ด PAM-4๋กœ ๊ฒฐํ•ฉํ•˜๋Š” ํšŒ๋กœ๊ฐ€ ์ œ์•ˆ๋œ๋‹ค. ๋‚ด๋ถ€ ๋ฐ ์ถœ๋ ฅ ๋…ธ๋“œ์—์„œ T-์ฝ”์ผ์€ ๋Œ€์—ญํญ์„ ์ฆ๊ฐ€์‹œํ‚ค๊ณ  ๊ธฐํ˜ธ ๊ฐ„ ๊ฐ„์„ญ(ISI)์„ ์ œ๊ฑฐํ•œ๋‹ค. ์ถœ๋ ฅ ๋„คํŠธ์›Œํฌ์—์„œ ์—ญํšŒ์ „ T-์ฝ”์ผ์€ T-์ฝ”์ผ์ด ์—†๋Š” ๊ฒฝ์šฐ๋ณด๋‹ค ๋Œ€์—ญํญ์„ 1.61๋ฐฐ ์ฆ๊ฐ€์‹œํ‚จ๋‹ค. VCSEL ๋“œ๋ผ์ด๋ฒ„๋Š” ์–‘๊ทน ๊ตฌ๋™ ๋ฐ ์ „๋ ฅ ๊ฐ์†Œ๋ฅผ ์œ„ํ•ด ๋†’์€ VSS ๋„๋ฉ”์ธ์— ๋ฐฐ์น˜๋œ๋‹ค. ์ด ์นฉ์€ 40 nm CMOS ๊ธฐ์ˆ ๋กœ ์ œ์ž‘๋˜์—ˆ๋‹ค. ์ œ์•ˆ๋œ VCSEL ์†ก์‹ ๊ธฐ๋Š” ๊ฐ๊ฐ 3.03pJ/b์™€ 2.09pJ/b์˜ ์ „๋ ฅ ํšจ์œจ๋กœ ์ตœ๋Œ€ 48Gb/s NRZ์™€ 64Gb/s PAM-4๊นŒ์ง€ ์ž‘๋™ํ•œ๋‹ค.ABSTRACT I CONTENTS III LIST OF FIGURES V LIST OF TABLES IX CHAPTER 1 INTRODUCTION 1 1.1 MOTIVATION 1 1.2 THESIS ORGANIZATION 5 CHAPTER 2 BACKGROUND OF HIGH-SPEED INTERFACE 6 2.1 OVERVIEW 6 2.2 BASIS OF DATA CENTER ARCHITECTURE 9 2.3 SHORT-REACH INTERFACE STANDARDS 12 2.4 ANALYSES OF BANDWIDTH EXTENSION TECHNIQUES 16 2.4.1 FRACTIONALLY-SPACED FFE 16 2.4.2 TRANSMISSION LINE 21 2.4.3 INDUCTOR 24 2.4.4 T-COIL 33 CHAPTER 3 DESIGN OF 48 GB/S PAM-4 ELECTRICAL TRANSMITTER IN 65 NM CMOS 43 3.1 OVERVIEW 43 3.2 FFE BASED ON DOUBLE-SHIELDED COPLANAR WAVEGUIDE 46 3.2.1 BASIC CONCEPT 46 3.2.2 PROPOSED DOUBLE-SHIELDED COPLANAR WAVEGUIDE 47 3.3 DESIGN CONSIDERATION ON 4:1 MUX 50 3.4 PROPOSED PAM-4 ELECTRICAL TRANSMITTER 53 3.5 MEASUREMENT 57 CHAPTER 4 DESIGN OF 64 GB/S PAM-4 OPTICAL TRANSMITTER IN 40 NM CMOS 64 4.1 OVERVIEW 64 4.2 DESIGN CONSIDERATION OF OPTICAL TRANSMITTER 66 4.3 PROPOSED PAM-4 VCSEL TRANSMITTER 69 4.4 MEASUREMENT 82 CHAPTER 5 CONCLUSIONS 88 BIBLIOGRAPHY 90 ์ดˆ ๋ก 101๋ฐ•

    Wideband integrated circuits for optical communication systems

    Get PDF
    The exponential growth of internet traffic drives datacenters to constantly improvetheir capacity. Several research and industrial organizations are aiming towardsTbps Ethernet and beyond, which brings new challenges to the field of high-speedbroadband electronic circuit design. With datacenters rapidly becoming significantenergy consumers on the global scale, the energy efficiency of the optical interconnecttransceivers takes a primary role in the development of novel systems. Furthermore,wideband optical links are finding application inside very high throughput satellite(V/HTS) payloads used in the ever-expanding cloud of telecommunication satellites,enabled by the maturity of the existing fiber based optical links and the hightechnology readiness level of radiation hardened integrated circuit processes. Thereare several additional challenges unique in the design of a wideband optical system.The overall system noise must be optimized for the specific application, modulationscheme, PD and laser characteristics. Most state-of-the-art wideband circuits are builton high-end semiconductor SiGe and InP technologies. However, each technologydemands specific design decisions to be made in order to get low noise, high energyefficiency and adequate bandwidth. In order to overcome the frequency limitationsof the optoelectronic components, bandwidth enhancement and channel equalizationtechniques are used. In this work various blocks of optical communication systems aredesigned attempting to tackle some of the aforementioned challenges. Two TIA front-end topologies with 133 GHz bandwidth, a CB and a CE with shunt-shunt feedback,are designed and measured, utilizing a state-of-the-art 130 nm InP DHBT technology.A modular equalizer block built in 130 nm SiGe HBT technology is presented. Threeultra-wideband traveling wave amplifiers, a 4-cell, a single cell and a matrix single-stage, are designed in a 250 nm InP DHBT process to test the limits of distributedamplification. A differential VCSEL driver circuit is designed and integrated in a4x 28 Gbps transceiver system for intra-satellite optical communications based in arad-hard 130nm SiGe process

    PAM4-๋ฐ”์ด๋„ˆ๋ฆฌ ๋ธŒ๋ฆฌ์ง€ ์นฉ์šฉ PAM4 ํŠธ๋žœ์Šค๋ฏธํ„ฐ ์„ค๊ณ„

    Get PDF
    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ) -- ์„œ์šธ๋Œ€ํ•™๊ต๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ์ „๊ธฐยท์ •๋ณด๊ณตํ•™๋ถ€, 2022. 8. ์ •๋•๊ท .๊ณ ์„ฑ๋Šฅ ์ปดํ“จํŒ… ์‹œ์Šคํ…œ, ๋Œ€์šฉ๋Ÿ‰์˜ ๋ฐ์ดํ„ฐ ์„ผํ„ฐ, AI ๊ธฐ์ˆ ์˜ ๋ฐœ์ „์œผ๋กœ ์ธํ•ด ์œ ์„  ํ†ต์‹ ์˜ ๋Œ€์—ญํญ ์š”๊ตฌ ์ˆ˜์ค€์€ ๊ธฐํ•˜๊ธ‰์ˆ˜์ ์œผ๋กœ ์ฆ๊ฐ€ํ•˜๊ณ  ์žˆ๋‹ค. ๊ทธ๋Ÿฌ๋‚˜ I/O ํšŒ๋กœ์˜ ํ•€๋‹น ๋Œ€์—ญํญ์˜ ํ–ฅ์ƒ์€ ํ†ต์‹  ์ฑ„๋„์˜ ๋‹ค์–‘ํ•œ ํ•œ๊ณ„๋กœ ์ธํ•ด ์–ด๋ ค์›€์„ ๊ฒช๊ณ  ์žˆ๋‹ค. ์ด๋Š” ์ฐจ์„ธ๋Œ€ DRAM ๋ถ„์•ผ์—์„œ๋„ ์˜ˆ์™ธ๋Š” ์•„๋‹ˆ๋‹ค. ํ•€๋‹น ๋ฐ์ดํ„ฐ ์ „์†ก ์†๋„๋ฅผ ์ฆ๊ฐ€์‹œํ‚ค๋Š” ์—ฐ๊ตฌ ๋ฐฉํ–ฅ์—์„œ๋Š” ์–ด๋Š ์ •๋„ ํ•œ๊ณ„์— ๋ด‰์ฐฉํ•˜๋ฉด์„œ ์ตœ๊ทผ์—๋Š” High Bandwidth Memory (HBM)์™€ ๊ฐ™์ด ํ•€์˜ ๊ฐœ์ˆ˜๋ฅผ ๊ธ‰๊ฒฉํžˆ ๋Š˜๋ ค์„œ ๋Œ€์—ญํญ์„ ์ฆ๊ฐ€์‹œํ‚ค๋Š” ๊ธฐ์ˆ ๋„ ๋ฐœ์ „ํ•˜๊ณ  ์žˆ๋‹ค. ๋‹ค๋ฅธ ์ ‘๊ทผ ๋ฐฉ์‹ ์ค‘ ํ•œ๊ฐ€์ง€๊ฐ€ ๋‹ค์ค‘ ๋ ˆ๋ฒจ ์‹ ํ˜ธ ๋ฐฉ์‹์ด๋‹ค. ๊ธฐ์กด์˜ Non-Return-to-Zero (NRZ) ์‹ ํ˜ธ ๋Œ€์‹ ์— ๋‹ค์ค‘ ๋ ˆ๋ฒจ ์‹ ํ˜ธ ๋ฐฉ์‹์„ ์ด์šฉํ•˜๋ฉด ๋™์ผํ•œ Nyquist ์ฃผํŒŒ์ˆ˜์—์„œ ๋ฐ์ดํ„ฐ ์†๋„๋ฅผ ๋†’์ผ ์ˆ˜ ์žˆ๊ณ  ์ด๋Š” DRAM์˜ ์ฐจ์„ธ๋Œ€ ๊ณ ๋Œ€์—ญํญ I/O ์ธํ„ฐํŽ˜์ด์Šค์— ์ข‹์€ ์†”๋ฃจ์…˜์ด ๋  ์ˆ˜ ์žˆ์œผ๋ฉฐ ํ˜„์žฌ๊นŒ์ง€๋Š” 4๋ ˆ๋ฒจ ํŽ„์Šค ์ง„ํญ ๋ณ€์กฐ ๋ฐฉ์‹ (PAM-4)์ด ๋„๋ฆฌ ์ฑ„ํƒ๋˜์–ด ์žˆ๋‹ค. ํ•˜์ง€๋งŒ ํ˜„์žฌ PAM-4 ๋ฐฉ์‹ DRAM์ด ์–‘์‚ฐ ๋‹จ๊ณ„๊ฐ€ ์•„๋‹ˆ๊ธฐ ๋•Œ๋ฌธ์— PAM-4 ์ „์šฉ Memory Tester๊ฐ€ ์—†๋Š” ์ƒํ™ฉ์ด๋‹ค. ๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์ฐจ์„ธ๋Œ€ ๋ฉ”๋ชจ๋ฆฌ ํ…Œ์ŠคํŠธ๋ฅผ ์œ„ํ•œ 32 Gb/s PAM4 ๋ฐ”์ด๋„ˆ๋ฆฌ ๋ธŒ๋ฆฌ์ง€์—์„œ์˜ ํŠธ๋žœ์Šค๋ฏธํ„ฐ๋ฅผ ์ œ์•ˆํ•œ๋‹ค. NRZ ํ…Œ์Šคํ„ฐ์—์„œ ๋ธŒ๋ฆฌ์ง€๋กœ ์ „์†ก๋œ ์ €์† ๋ฐ์ดํ„ฐ๋Š” ๊ณ ์† PAM4 ๋ฐ์ดํ„ฐ๋กœ ๋ณ€ํ™˜๋˜์–ด ๋ฉ”๋ชจ๋ฆฌ๋กœ ์ „๋‹ฌ๋œ๋‹ค. ์ ‘์ง€ ์ข…๋‹จ PAM4 ๋“œ๋ผ์ด๋ฒ„๋Š” 2-ํƒญ ํ”ผ๋“œํฌ์›Œ๋“œ ์ดํ€„๋ผ์ด์ €๋กœ ์ถœ๋ ฅ ์ „๋ฅ˜๋ฅผ ์ œ์–ดํ•˜์—ฌ 0.95์˜ ๋ ˆ๋ฒจ ๋ถˆ์ผ์น˜ ๋น„์œจ (RLM)์„ ๋‹ฌ์„ฑํ•จ์œผ๋กœ์จ ๋‹จ์ผ ์ข…๋‹จ ์ถœ๋ ฅ์„ ์ œ๊ณตํ•œ๋‹ค. 40 nm CMOS ๊ธฐ์ˆ ๋กœ ์ œ์ž‘๋œ ๋ธŒ๋ฆฌ์ง€ ํŠธ๋žœ์Šค๋ฏธํ„ฐ๋Š” 0.57 mm2์˜ ํ™œ์„ฑ ์˜์—ญ์„ ์ฐจ์ง€ํ•˜๊ณ  102.1 mW์˜ ์ „๋ ฅ์„ ์†Œ๋ชจํ•œ๋‹ค.With the advancement of high-performance computing systems, large-capacity data centers, and AI technologies, the level of bandwidth demand for wired communication is increasing exponentially. However, the improvement of the bandwidth per pin in the I/O circuit compared to the required bandwidth level is difficult due to various limitations of the transmission channel. This is no exception in the next generation of DRAM. While facing limitations from the perspective of research that increases data transmission speed per pin, technologies that increase I/O bandwidth by rapidly increasing the number of pins, such as High Bandwidth Memory (HBM), have also recently developed. One of the other approaches is a multi-level signaling method. Using a multi-level signaling method instead of a conventional Non-Return-to-Zero (NRZ) signal can increase data speed at the same Nyquist frequency, which can be a good solution for the next-generation high-bandwidth I/O interface of DRAM, and so far, a four-level Pulse Amplitude Modulation (PAM-4) has been widely adopted. However, since PAM4 DRAM is not in the mass production stage yet, there is no memory tester dedicated to PAM4 signaling. This paper proposes a transmitter block on a 32 Gb/s PAM4 binary bridge for next-generation memory testing. The low-speed data transmitted from the NRZ tester to the bridge is converted into high-speed PAM4 data through half-rate clock control and transferred to the memory. The ground termination PAM4 driver provides a single-ended output by controlling the output current with a two-tap feed forward equalizer to achieve a Level separation Mismatch Ratio (RLM) of 0.95. Bridge transmitter manufactured with 40 nm CMOS technology occupies an active area of 0.57 mm2 and consumes 102.1 mW of power.ABSTRACT I CONTENTS โ…ข LIST OF FIGURES โ…ค LIST OF TABLES โ…ฆ CHAPTER 1 INTRODUCTION 1 1.1 MOTIVATION 1 1.2 THESIS ORGANIZATION 4 CHAPTER 2 BACKGROUNDS 5 2.1 OVERVIEW 5 2.2 BASIC OF MULTI LEVEL SIGNALING 7 2.3 NECESSITY OF PAM4-BINARY BRIDGE 11 CHAPTER 3 DESIGN OF PAM4 TRANSMITTER FOR PAM4-BINARY BRIDGE 14 3.1 DESIGN CONSIDERATION 14 3.2 OVERALL ARCHITECTURE 17 3.3 CIRCUIT IMPLEMENTATION 19 3.3.1 CLOCK GENERATOR 19 3.3.2 PARALLEL PRBS GENERATOR 23 3.3.3 DATA ALIGN / GRAY CODE ENDCODER 26 3.3.4 FFE CONTROL/ SERIALIZER 30 3.3.5 PAM4 DRIVER 33 CHAPTER 4 MEASUREMENT RESULTS 38 4.1 CHIP PHOTOMICROGRAPH 38 4.2 MEASUREMENT SETUP 39 4.3 MEASUREMENT RESULTS 40 4.4 PERFORMANCE SUMMARY 42 CHAPTER 5 CONCLUSION 46 BIBLIOGRAPHY 47 ์ดˆ ๋ก 50์„

    50 GBd PAM4 transmitter with a 55nm SiGe BiCMOS driver and silicon photonic segmented MZM

    Get PDF
    We demonstrate an optical transmitter consisting of a limiting SiGe BiCMOS driver co-designed and co-packaged with a silicon photonic segmented traveling-wave Mach-Zehnder modulator (MZM). The MZM is split into two traveling-wave segments to increase the bandwidth and to allow a 2-bit DAC functionality. Two limiting driver channels are used to drive these segments, allowing both NRZ and PAM4 signal generation in the optical domain. The voltage swing as well as the peaking of the driver output are tunable, hence the PAM4 signal levels can be tuned and possible bandwidth limitations of the MZM segments can be partially alleviated. Generation of 50 Gbaud and 53 Gbaud PAM4 yields a TDECQ of 2.8 and 3.8 dB with a power efficiency of 3.9 and 3.6 pJ/bit, respectively; this is the best reported efficiency for co-packaged silicon transmitters for short-reach datacenter interconnects at these data rates. With this work, we show the potential of limiting drivers and segmented traveling-wave modulators in 400G capable short-reach optical interconnects
    • โ€ฆ
    corecore