Neal S. Bergano Tycom, Inc. Eatontown, NJ 07724ece-research.unm.edu/hayat/ece565/mod1.pdfNeal S....
Transcript of Neal S. Bergano Tycom, Inc. Eatontown, NJ 07724ece-research.unm.edu/hayat/ece565/mod1.pdfNeal S....
Introduction to Optical Communications
Thanks is due to slides from
Neal S. BerganoTycom, Inc.
Eatontown, NJ 07724
Neal S. BerganoTycom, Inc.
Eatontown, NJ 07724
Course Objectives
To develop a practical understanding of the components and techniques used in current optical communication systems and to have an analytical understanding of their capabilities and limitations.
Overview of the module
Outline -
Historical backgroundWhy Optical communications?Transmitting bits across the ocean using WDM techniques
A Brief History
1820: Oersted - Electricity deflects a magnet1831: Joseph Henry and Michael Faraday – elucidate laws of induction1838: Morse – telegraphy1858: First undersea cable Worked for 27 days
History
1865: Undersea cable laid between Canada and Ireland1876: Alexander Graham Bell invents the telephone1897: Marconi patents a wireless system
History
The Great Eastern deploys the first successful transatlantic telegraphcable in 1865. The cost of a message was $5 per word.
The Great Eastern deploys the first successful transatlantic telegraphcable in 1865. The cost of a message was $5 per word.
Bern Dibner, The Atlantic Cable, Burndy Library 1959
History
Undersea cable milestones:–1956 First Transatlantic Telephone Cable (TAT-1)
–1988 First Transatlantic Fiber Optic Cable (TAT-8)
–1998 First WDM Undersea Cable (AC-1)
Modern cable ship
Fiberoptics
Q Why fiberoptics?A Practical system designs have enormous
capacity (Hundreds of Gigabits per second)
Q Why do fiber systems support such large capacity?
A Optics provide very high frequency & bandwidth.
Old Trans-Atalantic cable
RESEARCH
DEPLOY
MANUFACTURE
TEST
DESIGN
MAINTAIN/ OPERATE
BranchingBranchingUnitUnit
RepeaterRepeater
CableCable
Traffic
Terminal
LineTerminatingEquipment
Power FeedEquipment
Undersea Network
Management Equipment
Cable geometry
OPTICALFIBER
UNITFIBER
STRUCTURE
STRENGTHWIRES
COPPERSHEATH
INSULATIONJACKET
ARMORED PROTECTIONLAYER
Cumulative Installed: Trans-Atlantic Capacity
Bit Rate Circuit Count*
(Gb/s) (# 64Kb/s)0.155 1,890 2.5 30,2405.0 60,48010 120,96040 483,840100 1,209,600160 1,935,360320 3,870,720
1000 12,096,000
Bit Rate Circuit Count*
(Gb/s) (# 64Kb/s)0.155 1,890 2.5 30,2405.0 60,48010 120,96040 483,840100 1,209,600160 1,935,360320 3,870,720
1000 12,096,000
1955 1965 1975 1985 1995
100
1K
10K
100K
1M
10M
NSB Atlanti2
1960 19801970 20001990
Dig
ital
Reg
ener
ator
s Opt
ical
Am
plifi
ers
20% AnnualGrowth
50% AnnualGrowth
64Kb/s Digital Circuits3KHz Analog Circuits
Analog
Repeaters
>100% Annual Growth
* Assuming:• 30 circuits per 2Mb/s E1• 63 E1s in an STM-1
YEAR
Four Generations of Lightwave Systems
First Generation: Digital regenerator, 1.3µm FP lasers, 1.3µm λ0 fiber. Example TAT-8, 0.3Gb/sFirst Generation: Digital regenerator, 1.3µm FP lasers, 1.3µm λ0 fiber. Example TAT-8, 0.3Gb/s
Second Generation: Digital regenerator, 1.55µm DFB lasers, 1.3µm λ0 fiber. Example TPC-4, 0.6Gb/sSecond Generation: Digital regenerator, 1.55µm DFB lasers, 1.3µm λ0 fiber. Example TPC-4, 0.6Gb/s
Third Generation: EDFA repeater, Single Channel, 1.55µm λ0 fiber. Example TAT12/13, 5 Gb/sThird Generation: EDFA repeater, Single Channel, 1.55µm λ0 fiber. Example TAT12/13, 5 Gb/s
Fourth Generation: EDFA repeater, Multi Channel, 1.58µm λ0 fiber. Example AC1, 16x2.5 Gb/sFourth Generation: EDFA repeater, Multi Channel, 1.58µm λ0 fiber. Example AC1, 16x2.5 Gb/s
The Early 1990’s Capacity Dilemma
Optical fibers have a large intrinsic capacity, but fiber opticsystems using electro-optic regenerators do not.
Optical fibers have a large intrinsic capacity, but fiber opticsystems using electro-optic regenerators do not.
Optical amplifier repeaters(Remove capacity bottleneck)
Wavelength division multiplexing(Use more bandwidth)
Dispersion management(Reduce channel interactions)
New transmission formats(Allow for higher data rates)
Forward error correcting codes(Improve error performance)
Time
Undersea fiberoptic cable systems make the Web “Worldwide”
Data Waveforms
Bit Slot = 94 psec (10.7 Gb/s signal)Bit Slot = 94 psec (10.7 Gb/s signal)
Equivalent distance traveled in a fiber (one bit is 0.75in long in a fiber)
Equivalent distance traveled in a fiber (one bit is 0.75in long in a fiber)
Non-Return-to-Zero (NRZ) and Return-to-Zero (RZ) is a uni-polar binary code. Binary “1” is represented with a pulse, and “0” is represented by the absence of a pulse.
T=1/B
T=1/B
NRZRZ
Soliton
Inte
nsity
Time
Data streams
NRZ
CRZ
Soliton
Time
1 1 1 0 11 101
Bit Slot
Frequency/Bandwidth
540kHz 1600kHz
AM radio(10KHz)
Sports radio 660 Bloomberg 1130
. . .
Infrared
Light(10GB/s)
230 THz(1300nm)
190 THz(1600nm)
450 THz(660nm)
Red
Ora
nge
Yello
wG
reen
Blue
Indi
goVi
olet
100 Million times
Capacity
Light
40 THz
230 THz(1300nm)
190 THz(1600nm)
450 THz(660nm)
Today’s optical fiber has a potential of about 40Tera Hz of “Bandwidth” {40,000,000,000,000Hz}If we could use 1/2 of the available bandwidth, the ultimate capacity of a fiberoptic transmission system would be about 20TB/s20TB/s is equivalent to 1/2 Billion 45KBit/s modem connections
Red
Ora
nge
Yello
wG
reen
Blue
Indi
goVi
olet
C-Band EDFA191.7 - 196.7 THz
(5THz)
Chromatic Dispersion
Different wavelengths travel at different speed, or group velocity.
Example: 50km of standard single mode fiber
Time Delay
Wavelength
244.4 usec
1550.0 1550.8
Equivalent fiber length
50 km
50 km + 14cm244.40068usec
Signal Distortion Caused by Chromatic Dispersion
Eye Diagram Optical Spectrum
Chromatic Dispersion: Different wavelengths travel at different speed, or group velocity.
The Early 1990’s Capacity Dilemma
Optical fibers have a large intrinsic capacity, but fiber opticsystems using electro-optic regenerators do not.
Optical fibers have a large intrinsic capacity, but fiber opticsystems using electro-optic regenerators do not.
T R
Electro-Optic Repeater
Erbium-doped Fiber Amplifier
PumpLaser
Pump/SignalCombiner
ErbiumFiber
(10-50 m)
Distortionless Amplification of Light
Bit-Rate Independent
Signal Remains in Fiber
Amplifies Many Wavelengths Simultaneously
Transmitting bits through a fiberoptic line
OpticalTransmitter
OpticalReceiverBPF
Data source
DataSink
1 1 1 0 1 0 10 0 11
Optical Amplifier Transmission System
T RBPF
Single Channel
Wavelength Division MultiplexingλN
λ3
λ2
λ1
RBPF
RBPF
RBPF
RBPFλN
λ3
λ2
λ1T
T
T
T
Wavelength Division Multiplexing (WDM)
Data bits in the fiber
λN
λ3
λ2
λ1T
T
T
T
Project Yellow:• 32 x 10Gb/s channels• Channel spacing is
0.6nm (or 75GHz)
Optical Spectrum
Intensity
(or brightness)
Wavelength (color)
Amplified Transmission Line
g
1/g
g
1/g
g
1/g
Operating Point
AmplifierGain
Output Power
(Span Loss)-1
Gain Compression
3.0
2.5
2.0
1.5
1.0
0.5
0.00 2000 4000 6000 8000 10000
Distance (km)
Opt
ical
Pow
er (m
W)
Signal Power
Noise Power
Noise Accumulation In Amplifier Systems
gg ++2nsp(g-1)hvB0
Pin Pout
30 dB Amplifier: 400µW/A in 10,000km
150 km10 dB Amplifier: 12µW/A in 10,000km
Transmission Formats
Old Thinking:
NRZ had the advantage of compatibility, with adequate performance.
Solitons had the advantage of single channel capacity.
Use NRZ first, than switch to a “higher” capacity format.
Old Thinking:
NRZ had the advantage of compatibility, with adequate performance.
Solitons had the advantage of single channel capacity.
Use NRZ first, than switch to a “higher” capacity format.
What has happened over the past 5 years:
WDM removed the capacity advantage of solitons.
NRZ migrated to synchronously modulated NRZ.
Solitons migrated to guided, dispersion managed solitons.
What has happened over the past 5 years:
WDM removed the capacity advantage of solitons.
NRZ migrated to synchronously modulated NRZ.
Solitons migrated to guided, dispersion managed solitons.
Present Thinking: Increase capacity using WDM
Reduce and/or manage the fiber’s nonlinear index
Take advantage of fiber’s nonlinear index
Present Thinking: Increase capacity using WDM
Reduce and/or manage the fiber’s nonlinear index
Take advantage of fiber’s nonlinear index
WDM Transmitter
Chirped Return-to-Zero (CRZ) Signal
...
Com
bine
rC
ombi
ner
Com
bine
r111
333
636363
DataDataData
time
Phase
Intensity
time
220-1222020--11FECFECFEC
...
Com
bine
rC
ombi
ner
Com
bine
r222
444
646464
DataDataData AMAMAM PMPMPM
215-1221515--11FECFECFEC
AMAMAM PMPMPM
CRZ Waveform: More tolerant to large accumulated dispersion
CRZ Waveform: More tolerant to large accumulated dispersion
λ
... ...Orthogonal polarization launch: Reduced channel interaction
Basic definitions
Losses in dB
X dB = -10 log10 (Pout/Pin)
Beer’s law : Pout/Pin = e-αL
dB/Km =X/L= 10 log10 (e) α
Power (dBm) = 10 log10 (P(mW)/1 mW)
Log(Pin)
Distance
Signal digitizing
Sampling theorem due to Nyquist
sample frequency
fs > 2 ∆f
∆f is the signal bandwidth
Digital signal has finite accuracy,
say m bits. The number of quantized
levels is M = 2m
Digitized Signal
Bandwidth of digital signal B = m fsSignal to noise ratio (SNR)
SNR (dB) = 20 log10 (Amax/AN)
M > Amax/AN
AN is the average noise amplitude
B > 2 ∆f log10(M)/ log10(2) > ∆f SNR/3