34
Nortel Confidential Information BUSINESS MADE SIMPLE 1 DSP A Disruptive Technology for Optical Transceivers Kim Roberts Ian Roberts

DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

  • Upload
    others

  • View
    0

  • Download
    0

Embed Size (px)

Citation preview

Page 1: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

Nortel Confidential Information

BUSINESS MADE SIMPLE

1

DSPA Disruptive Technologyfor Optical Transceivers

Kim RobertsIan Roberts

Page 2: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

2

NoiseLimited

Transmission

> Early fibers had losses measured in dB/meter> Given the very finite amount of optical power that could be

coupled into the fibers, received powers quickly became very low.

> Thermal noise in the receiver limited the bandwidth and distance for optical transmission.• E.g. 1 Mb/s along 10 meters, experiments at Harlow Labs

Page 3: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

FD-135 used Duobinary Coding in 1983to mitigate Modal Dispersion on

Multimode fiber

Proakis, Digital Communications

Page 4: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

SuperDecoder

Page 5: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

Decision Feedback

Winters et al, IEEE Communications Magazine, June 1993

Page 6: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

6

Forward Error Correction to Mitigate Noise

1 2 3 4 5 6 7 810

−15

10−10

10−5

100

Uncoded

Q

BE

R

Uncoded

1 2 3 4 5 6 7 810

−15

10−10

10−5

100

Uncoded

Q

BE

R

BCH−1BCH-1

Uncoded

1 2 3 4 5 6 7 810

−15

10−10

10−5

100

Uncoded

Q

BE

R

BCH−1

BCH−3BCH-3

BCH-1

Uncoded

1 2 3 4 5 6 7 810

−15

10−10

10−5

100

Uncoded

Q

BE

R

BCH−1

BCH−3RSG.975 BCH-3

BCH-1

Uncoded

1 2 3 4 5 6 7 810

−15

10−10

10−5

100

Uncoded

Q

BE

R

BCH−1

BCH−3RS

BCH−20

G.975

BCH-20

BCH-3

BCH-1

Uncoded

1 2 3 4 5 6 7 810

−15

10−10

10−5

100

Uncoded

Q

BE

R

BCH−1

BCH−3RS

BCH−20BCH−2⊗BCH−3

G.975

P-FECBCH-20

BCH-3

BCH-1

Uncoded

Peak Signal to RMS Noise Ratio

Log

Bit

Erro

r Rat

e af

ter F

EC

Page 7: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

7

Traditional Solution for Dispersion:Optical Compensation Modules

Page 8: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

Maximum Likelihood Sequence EstimationMLSE

> M.Cavallari, C.R.S.Fludger, P.J.Anslow, Electronic signal processing for differential phase modulation formats, Optical Fiber Communication Conference, (Feb 2004)

Page 9: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

Coherent to the E-Field

> Major sources of degradation are linear with respect to the optical E-field.• Linear and invertible functions• Linear functions are commutative

> Linear transducers can be built• Digital to E-field• E-field to digital

> Therefore, linear digital filtering can fully compensate

Page 10: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

Linear Conversion from Digital to E-Field

Page 11: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

11

Dispersion Eliminator: WARP ASIC

0.13 μm BiCMOS

2.5 Mb High Speed Memory2.0 M Gates

6 T Ops per second

Two 20 Gs/s 6 bit DAC

17 Watts

Linear and nonlinear pre-compensation of 10 Gb/s±80,000 ps/nm (2 dB penalty point)

Page 12: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

12

Dispersion Precompensation

Signal Transmitted Signal after 1600 km of NDSFWith no optical compensation.

Page 13: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

13

10 Gb/swith no Traditional Dispersion Compensation

Eye diagrams after transmission over standard G.652 fiber with Nortel WARP processing.

0 Km 1600 km 3200 km 5120 km

Page 14: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

14

SPM Precompensation, 1280 km

5.0

7.0

9.0

11.0

13.0

15.0

-5.0 -3.0 -1.0 1.0 3.0 5.0

Average Launch Power dBm

Req

uire

d O

SNR

at 1

E-3 Linear Compensation Only

With SPM CompensationReference Line

Page 15: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

15

E-Field to Digital Transducer

> Two phases: Real and Imaginary (I and Q)• Best detected by mixing with a local oscillator

> Two polarizations

> Four dimensions fully span the E-field in a single mode fiber.

Page 16: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

16

Coherent Detection

QX Pol

I

I Y Pol

Q

Page 17: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

17

Page 18: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

18

A/D and Filter ASIC

90 nm CMOS

20 M Gates

12 T Ops per second

Four 20 Gs/s 6 bit ADC

21 Watts

Linear and nonlinear post-compensation of 40 Gb/s±80,000 ps/nm, 25 ps mean PMD, 2 dB mean PDL

Page 19: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

19

40G/100G Agile Optical EngineBinary to dual polarization E-field

Full E-field to Digital Transducer

Page 20: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

20

40 Gb/s Coherent Dual Pol QPSK Modem

Page 21: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

Real-time PMD tracking> 1000 km of NDSF

> 10G, 40G, and 100G at 50 GHz spacing

> JDS PMD emulator

Page 22: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

22

PMD Tracking

Page 23: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

2323

100G Dual Carrier

10G10GeDCO eDCO

AgileAgile100G100G

AgileAgile40G40G

Page 24: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

24

100 Gb/sModem

Page 25: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

200G, 400G, 1000G

>Lower cost per bit

>More bits per fiber

>Larger packet streams

(From here on are my personal speculations and not product delivery commitments.)

Page 26: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

Lightpath Bit Rate

The bit rate is the product of three dimensions

Page 27: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

More Symbols per Second

>Faster A/D•11, 28, 56, … GBaud

>More gates of DSP

>CMOS riding Moore’s Law• Bipolar is too hot and does not have the gate count

Page 28: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

Electronics for Processing

Page 29: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

More Bits per Symbol

-2 -1 0 1 2-2.5

-2

-1.5

-1

-0.5

0

0.5

1

1.5

2

2.5

DP 16-QAM

4 bits x 2 Pol=8 bits per Baud

x 28.5 Gbaud= 228 Gb/s

I

Q

Page 30: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

● 40 G

Spectral Efficiency

20

0.2

2

6

0.8

● 10 G

● 100 G

Spectral Efficiency is ultimately determined by OSNR

“The Channel Capacity of a Multispan DWDM System Employing Dispersive Nonlinear Optical Fibers and an Ideal Coherent Optical Receiver”, Jau Tang, JLT, Vol. 20, No. 7, July 2002

Page 31: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

Multiple Carriers

>Coherent Frequency Selection• Two carriers with 16-QAM = 400 Gb/s

>OFDM

>New ideas are needed

Page 32: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

OFDM

> Jolley et al, OFC 2005

> First Optical OFDM: Multimode fiber in Nortel lab.

Page 33: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

Spectral Efficiency

Year of Product Introduction

Tb/sinC Band

Bits/sperHz

1995 2000 2005 2010 Future…0

1

2

3

4

0

5

10

15

20

● 10G10.7 Gb/s @ 50 GHz

● 46 Gb/s @ 50 GHz

112 Gb/s @ 50 GHz ●

224 Gb/s @ 50 GHz ●

448 Gb/s @ 80 GHz ●

525

1000 Gb/s @ 170 GHz ●6

Page 34: DSP A Disruptive Technology for Optical TransceiversKim Roberts Ian Roberts 2 Noise Limited Transmission >Early fibers had losses measured in dB/meter >Given the very finite amount

100G Dual Carrier Real Time Data> 1000 km of NDSF

> 10G, 40G, and 100G at 50 GHz spacing

> JDS PMD emulator