3
12 2012 IEEE International Solid-State Circuits Conference ISSCC 2012 / SESSION 24 / 10G BASET & OPTICAL FRONTENDS / 24.4 24.4 A 10Gb/s Burst-Mode TIA with On-Chip Reset/Lock CM Signaling Detection and Limiting Amplifier with a 75ns Settling Time Xin Yin 1 , Jasmien Put 1 , Jochen Verbrugghe 1 , Jan Gillis 1 , Xing-Zhi Qiu 1 , Johan Bauwelinck 1 , Jan Vandewege 1 , Heinz-Georg Krimmel 2 , Mohand Achouche 3 1 imec - Ghent University, Gent, Belgium 2 Bell Laboratories, Stuttgart, Germany 3 III-V Lab, Marcoussis, France Emerging symmetric 10Gb/s passive optical network (PON) systems aim at high network transmission efficiency by reducing the RX settling time that is needed for RX amplitude recovery in burst-mode (BM). A conventional AC-coupled BM- RX has an inherent tradeoff between short settling time and decision threshold droop, which makes an RX settling time shorter than 400ns hard to achieve [1]. Some techniques have been developed to overcome this limitation [1-2], demon- strating a settling time of 150 to 200ns. Our previous work [3] uses feed-forward automatic offset compensation (AOC) to achieve a response time as short as 25.6ns. However, a feed-forward scheme using peak detectors is intrinsically less accurate and results in relatively high power consumption. In this paper, we present a DC-coupled 10Gb/s BM-TIA and burst-mode limiting amplifier (BM- LA) chipset that uses a feedback type AOC circuit with switchable loop BW. This new technique is capable of removing input DC offset in less than 75ns, and offers continuous decision threshold tracking during payload, to cope with the maximum length of CID. The differential TIA output port senses a CM reset sig- nal provided by the succeeding BM-LA, and activates an on-chip reset and lock function. This BM-LA also integrates auto reset/activity generation circuits pro- viding the AOC BW switching signal, so that this time-critical signal is not required from the PON system. The chipset’s top-level architecture is shown in Fig. 24.4.1. When a burst arrives, BM-TIA performs a fast three-step gain switch (GS) while the activity detection circuit in BM-LA detects the start of the incoming burst. During the preamble, the offset integrator increases the AOC loop BW to achieve fast settling. The AOC BW is then switched to a smaller value, for continuous decision threshold track- ing during the payload. At the end-of-burst, the BM-LA resets itself to its initial state preparing for the next burst to come. The BM-LA also sends the reset/activ- ity signal back to the preceding BM-TIA IC by driving the input common-mode voltage V CM . The BM-TIA extracts reset and gain lock signals from V CM without any performance penalty. As shown in Fig. 24.4.2, the BM-TIA reset/lock CM detection circuit contains CM extraction, a differentiator, two comparators and a RS latch with a delayed out- put. The differentiator is a passive HPF circuit converting the square wave V CM into high frequency spikes V DF . A reset pulse is generated via comparison to V REF2 at the V CM falling edge. At the V CM rising edge, when the positive spike V DF crosses the threshold voltage V TH1 , the RS latch sets the lock after an addition- al delay T GS for gain switch settling. The R DF C DF time constant is made short compared to the burst guard time but large enough to generate the reset pulse robustly over PVT corners. Because of simultaneous DM and CM signaling at the 10Gb/s BM-TIA output, mode conversions between DM and CM must be taken into account as the conversion ratio can be significant in the GHz frequency range. Since V CM only switches during the guard time and the preamble period, CM-to-DM conversion is no problem when the data payload is received. However, DM-to-CM conversion, partly due to mismatches in PCB conductor lengths and loading conditions, generates CM noise that might cause false gain reset/lock signaling. Therefore an LPF capacitor, C, is inserted in the CM extrac- tion circuit, and the comparators are implemented as two-stage amplifiers with an output LPF (formed by R 2 and C 2 ) to remove high-frequency CM ripple. In BM-LA, instead of using a RC low-pass filter in the AOC [4], the offset is can- celled by means of an offset integrator (Fig. 24.4.3) loop with adjustable loop BW. For small signals, the AOC loop BW is proportional to the unity-gain fre- quency of the integrator ~ gm/C L . As the transconductance of the input differen- tial pairs (Q 1 -Q 2 for V 1+/- and Q 3 -Q 4 for V 2+/- ) scales with the emitter current, the loop BW can be adapted by changing the tail currents I ss1 and I ss2 . In BM oper- ation, the control logic clears the charge accumulated in the integrator with a PMOS switch M 5 during the guard time between bursts. It also generates a switching signal to control the AOC loop BW. When BW_Switch is high, the off- set integrator has a large AOC loop BW due to a large tail current. When BW_Switch is low, the tail current is reduced and so the small loop BW mini- mizes the data-dependent jitter. As shown in Fig. 24.4.3, the control logic de- asserts the Clear signal when activity is high, and asserts it when reset is high; the BW_Switch replicates the Clear signal, with an additional T settling delay as required for the BM-LA AOC settling. The auto reset/activity circuits were designed to accommodate new require- ments of emerging 10G-GPONs: a FEC code is now mandatory in order to extend the optical power budget. In previous work [5], the reset generation circuit measured the time since the last received “1” level, and a reset was generated when this time exceeded the longest CID time. Although this technique works well at low BER (e.g. 10 -10 ), it starts to miss resets when the BER rises. In the new reset generation circuit (Fig. 24.4.4), two counters, a data counter and a clock counter, count the number of rising edges of the data stream (V 3 ) and the clock signal ClockLS, respectively. ClockLS has a clock period of the duration of the maximum CID. The data counter is compared to CountData, which repre- sents the number of bit errors allowed during the auto-reset generation. The clock counter is compared to CountClk, which defines the data counting time. Both CountData and CountClk are programmable. When no more than CountData rising edges occur before CountClk clock periods expire, a reset sig- nal is generated. In this way it is avoided that a reset is missed in case one or a few bits would be wrong at a pre-FEC BER [6]. The BM-TIA and BM-LA ICs are fabricated in a 0.13μm SiGe BiCMOS process. The BM-TIA and BM-LA consume 200 and 430mW, respectively, at 2.5V and 2.2V. Figure 24.4.5 shows BM-TIA output, BM-LA output and reset/activity CM signaling waveforms. Figure 24.4.6 shows the measured BERs with and without an off-chip reset signal. With an off-chip reset signal, the measured BM-RX set- tling time is 50ns over the whole input optical power range (-5dBm down to -31.2dBm). Allowing for 75ns of settling time, the sensitivity penalty from using the on-chip reset/activity generation instead of an off-chip reset signal is limited to 0.4dB at BER = 10 -10 . The eye diagrams in Fig. 24.4.6 prove the superior CID tolerance: after 64-, 128- and 512-bit CID, the measured total jitter J pp is 22.7ps, 23.1ps, and 23.8ps respectively. Fig. 24.4.7 shows die micrographs. The BM-TIA occupies 1.28×1.02mm 2 and the BM-LA occupies 1.21×.26mm 2 . Acknowledgement: This work was supported by the FP7 ICT projects MARISE and EURO-FOS. The authors thank Sumitomo Electric Devices Innovations, Inc for APD-TIA ROSA assembly and STMicroelectronics for chip fabrication. References: [1] K. Hara, et al., “New AC-Coupled Burst-Mode Optical Receiver Using Transient-Phenomena Cancellation Techniques for 10 Gbit/s-Class High-Speed TDM-PON Systems,” IEEE/OSA Journal of Lightwave Technology, pp. 2775- 2782, Oct. 2010. [2] M. Nogawa, et al., “A 10-Gb/s Burst-mode Limiting Amplifier Using a Two- stage Active Feedback Circuit”, Symp. on VLSI Circuits Dig. Tech. Papers, pp. 18-19, June 2009. [3] T. De Ridder, et al., “10 Gbit/s burst-mode post-amplifier with automatic reset,” Electron. Lett., pp. 1371-1373, Nov. 2008. [4] K-C. Wu, et al., “A 2x25Gb/s deserializer with 2:5 DMUX for 100Gb/s ether- net applications,” ISSCC Dig. Tech. Papers, pp. 374-375, Feb. 2010. [5] C. Mélange, et al., “Fully DC-Coupled 10Gb/s Burst-Mode PON Prototypes and Upstream Experiments with 58ns Overhead,” Optical Fiber Communication Conf. Proc. pp. OWX2, Mar. 2010. [6] C. Mélange, et al., “Circuit for End-of-Burst Detection,” US patent application US 2011/0069952 A1. 978-1-4673-0377-4/12/$31.00 ©2012 IEEE Session_24_Digest 11/29/11 1:13 PM Page 12

Session 24 Digest · ISSCC 2012 / SESSION 24 / 10G BASET & OPTICAL FRONTENDS / 24.4 24.4 A 10Gb/s Burst-Mode TIA with On-Chip Reset/Lock CM Signaling Detection and Limiting Amplifier

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Page 1: Session 24 Digest · ISSCC 2012 / SESSION 24 / 10G BASET & OPTICAL FRONTENDS / 24.4 24.4 A 10Gb/s Burst-Mode TIA with On-Chip Reset/Lock CM Signaling Detection and Limiting Amplifier

12 • 2012 IEEE International Solid-State Circuits Conference

ISSCC 2012 / SESSION 24 / 10G BASET & OPTICAL FRONTENDS / 24.4

24.4 A 10Gb/s Burst-Mode TIA with On-Chip Reset/Lock CM Signaling Detection and Limiting Amplifier with a 75ns Settling Time

Xin Yin1, Jasmien Put1, Jochen Verbrugghe1, Jan Gillis1, Xing-Zhi Qiu1, Johan Bauwelinck1, Jan Vandewege1, Heinz-Georg Krimmel2, Mohand Achouche3

1imec - Ghent University, Gent, Belgium2Bell Laboratories, Stuttgart, Germany3III-V Lab, Marcoussis, France

Emerging symmetric 10Gb/s passive optical network (PON) systems aim at highnetwork transmission efficiency by reducing the RX settling time that is neededfor RX amplitude recovery in burst-mode (BM). A conventional AC-coupled BM-RX has an inherent tradeoff between short settling time and decision thresholddroop, which makes an RX settling time shorter than 400ns hard to achieve [1].Some techniques have been developed to overcome this limitation [1-2], demon-strating a settling time of 150 to 200ns. Our previous work [3] uses feed-forwardautomatic offset compensation (AOC) to achieve a response time as short as25.6ns. However, a feed-forward scheme using peak detectors is intrinsicallyless accurate and results in relatively high power consumption. In this paper, wepresent a DC-coupled 10Gb/s BM-TIA and burst-mode limiting amplifier (BM-LA) chipset that uses a feedback type AOC circuit with switchable loop BW. Thisnew technique is capable of removing input DC offset in less than 75ns, andoffers continuous decision threshold tracking during payload, to cope with themaximum length of CID. The differential TIA output port senses a CM reset sig-nal provided by the succeeding BM-LA, and activates an on-chip reset and lockfunction. This BM-LA also integrates auto reset/activity generation circuits pro-viding the AOC BW switching signal, so that this time-critical signal is notrequired from the PON system.

The chipset’s top-level architecture is shown in Fig. 24.4.1. When a burst arrives,BM-TIA performs a fast three-step gain switch (GS) while the activity detectioncircuit in BM-LA detects the start of the incoming burst. During the preamble,the offset integrator increases the AOC loop BW to achieve fast settling. The AOCBW is then switched to a smaller value, for continuous decision threshold track-ing during the payload. At the end-of-burst, the BM-LA resets itself to its initialstate preparing for the next burst to come. The BM-LA also sends the reset/activ-ity signal back to the preceding BM-TIA IC by driving the input common-modevoltage VCM. The BM-TIA extracts reset and gain lock signals from VCM withoutany performance penalty.

As shown in Fig. 24.4.2, the BM-TIA reset/lock CM detection circuit contains CMextraction, a differentiator, two comparators and a RS latch with a delayed out-put. The differentiator is a passive HPF circuit converting the square wave VCMinto high frequency spikes VDF. A reset pulse is generated via comparison toVREF2 at the VCM falling edge. At the VCM rising edge, when the positive spike VDFcrosses the threshold voltage VTH1, the RS latch sets the lock after an addition-al delay TGS for gain switch settling. The RDFCDF time constant is made shortcompared to the burst guard time but large enough to generate the reset pulserobustly over PVT corners. Because of simultaneous DM and CM signaling at the10Gb/s BM-TIA output, mode conversions between DM and CM must be takeninto account as the conversion ratio can be significant in the GHz frequencyrange. Since VCM only switches during the guard time and the preamble period,CM-to-DM conversion is no problem when the data payload is received.However, DM-to-CM conversion, partly due to mismatches in PCB conductorlengths and loading conditions, generates CM noise that might cause false gainreset/lock signaling. Therefore an LPF capacitor, C, is inserted in the CM extrac-tion circuit, and the comparators are implemented as two-stage amplifiers withan output LPF (formed by R2 and C2) to remove high-frequency CM ripple.

In BM-LA, instead of using a RC low-pass filter in the AOC [4], the offset is can-celled by means of an offset integrator (Fig. 24.4.3) loop with adjustable loopBW. For small signals, the AOC loop BW is proportional to the unity-gain fre-quency of the integrator ~ gm/CL. As the transconductance of the input differen-tial pairs (Q1-Q2 for V1+/- and Q3-Q4 for V2+/-) scales with the emitter current, the

loop BW can be adapted by changing the tail currents Iss1 and Iss2. In BM oper-ation, the control logic clears the charge accumulated in the integrator with aPMOS switch M5 during the guard time between bursts. It also generates aswitching signal to control the AOC loop BW. When BW_Switch is high, the off-set integrator has a large AOC loop BW due to a large tail current. WhenBW_Switch is low, the tail current is reduced and so the small loop BW mini-mizes the data-dependent jitter. As shown in Fig. 24.4.3, the control logic de-asserts the Clear signal when activity is high, and asserts it when reset is high;the BW_Switch replicates the Clear signal, with an additional Tsettling delay asrequired for the BM-LA AOC settling.

The auto reset/activity circuits were designed to accommodate new require-ments of emerging 10G-GPONs: a FEC code is now mandatory in order to extendthe optical power budget. In previous work [5], the reset generation circuitmeasured the time since the last received “1” level, and a reset was generatedwhen this time exceeded the longest CID time. Although this technique workswell at low BER (e.g. 10-10), it starts to miss resets when the BER rises. In thenew reset generation circuit (Fig. 24.4.4), two counters, a data counter and aclock counter, count the number of rising edges of the data stream (V3) and theclock signal ClockLS, respectively. ClockLS has a clock period of the duration ofthe maximum CID. The data counter is compared to CountData, which repre-sents the number of bit errors allowed during the auto-reset generation. Theclock counter is compared to CountClk, which defines the data counting time.Both CountData and CountClk are programmable. When no more thanCountData rising edges occur before CountClk clock periods expire, a reset sig-nal is generated. In this way it is avoided that a reset is missed in case one or afew bits would be wrong at a pre-FEC BER [6].

The BM-TIA and BM-LA ICs are fabricated in a 0.13µm SiGe BiCMOS process.The BM-TIA and BM-LA consume 200 and 430mW, respectively, at 2.5V and2.2V. Figure 24.4.5 shows BM-TIA output, BM-LA output and reset/activity CMsignaling waveforms. Figure 24.4.6 shows the measured BERs with and withoutan off-chip reset signal. With an off-chip reset signal, the measured BM-RX set-tling time is 50ns over the whole input optical power range (-5dBm down to -31.2dBm). Allowing for 75ns of settling time, the sensitivity penalty from usingthe on-chip reset/activity generation instead of an off-chip reset signal is limitedto 0.4dB at BER = 10-10. The eye diagrams in Fig. 24.4.6 prove the superior CIDtolerance: after 64-, 128- and 512-bit CID, the measured total jitter Jpp is 22.7ps,23.1ps, and 23.8ps respectively. Fig. 24.4.7 shows die micrographs. The BM-TIAoccupies 1.28×1.02mm2 and the BM-LA occupies 1.21×.26mm2.

Acknowledgement:This work was supported by the FP7 ICT projects MARISE and EURO-FOS. Theauthors thank Sumitomo Electric Devices Innovations, Inc for APD-TIA ROSAassembly and STMicroelectronics for chip fabrication.

References: [1] K. Hara, et al., “New AC-Coupled Burst-Mode Optical Receiver UsingTransient-Phenomena Cancellation Techniques for 10 Gbit/s-Class High-SpeedTDM-PON Systems,” IEEE/OSA Journal of Lightwave Technology, pp. 2775-2782, Oct. 2010.[2] M. Nogawa, et al., “A 10-Gb/s Burst-mode Limiting Amplifier Using a Two-stage Active Feedback Circuit”, Symp. on VLSI Circuits Dig. Tech. Papers, pp.18-19, June 2009.[3] T. De Ridder, et al., “10 Gbit/s burst-mode post-amplifier with automaticreset,” Electron. Lett., pp. 1371-1373, Nov. 2008. [4] K-C. Wu, et al., “A 2x25Gb/s deserializer with 2:5 DMUX for 100Gb/s ether-net applications,” ISSCC Dig. Tech. Papers, pp. 374-375, Feb. 2010. [5] C. Mélange, et al., “Fully DC-Coupled 10Gb/s Burst-Mode PON Prototypesand Upstream Experiments with 58ns Overhead,” Optical Fiber CommunicationConf. Proc. pp. OWX2, Mar. 2010.[6] C. Mélange, et al., “Circuit for End-of-Burst Detection,” US patent applicationUS 2011/0069952 A1.

978-1-4673-0377-4/12/$31.00 ©2012 IEEE

Session_24_Digest 11/29/11 1:13 PM Page 12

Page 2: Session 24 Digest · ISSCC 2012 / SESSION 24 / 10G BASET & OPTICAL FRONTENDS / 24.4 24.4 A 10Gb/s Burst-Mode TIA with On-Chip Reset/Lock CM Signaling Detection and Limiting Amplifier

13DIGEST OF TECHNICAL PAPERS •

ISSCC 2012 / February 22, 2012 / 4:15 PM

Figure 24.4.1: Top level architecture of BM-TIA and BM-LA. Figure 24.4.2: CM signaling detection circuit.

Figure 24.4.3: Offset integrator with switchable loop BW.

Figure 24.4.5: BM-TIA output, BM-LA output and reset/activity CM signalingwaveforms. Figure 24.4.6: Measured BERs and total jitters.

Figure 24.4.4: On-chip reset generation.

24

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Page 3: Session 24 Digest · ISSCC 2012 / SESSION 24 / 10G BASET & OPTICAL FRONTENDS / 24.4 24.4 A 10Gb/s Burst-Mode TIA with On-Chip Reset/Lock CM Signaling Detection and Limiting Amplifier

14 • 2012 IEEE International Solid-State Circuits Conference 978-1-4673-0377-4/12/$31.00 ©2012 IEEE

ISSCC 2012 PAPER CONTINUATIONS

Figure 24.4.7: Die micrograph of BM-TIA and BM-LA.

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