innovative modulation schemes for future optical wdm ... · wr, apoc 2003; slide 1 chair for...
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wr, APOC 2003; slide 1
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Innovative Modulation Schemes for Future Optical WDM-Transmission
Werner RosenkranzThanks to: Jochen Leibrich, Murat Serbay, Christoph Wree,
Torsten Wuth, Maike Wichers
University of Kiel, Germany
Chair for CommunicationsKaiserstr. 2, 24143 Kiel, Germany
Email: [email protected]
wr, APOC 2003; slide 2
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Introduction
Innovative modulation formats have impact on transmission
performance of optical networks.
They may:
+ increase bandwidth efficiency (i.e. narrowing of channel
spacing)
+ increase transmission span reach
+ increase system margin and tolerances
– increase system complexity and equipment cost
– not be in compliance with existing standards
wr, APOC 2003; slide 3
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Outline
1. Introduction
2. Modulation of Optical Carriers
3. Options for Alternative Modulation Formats
a. Duobinary Signaling
b. Single Sideband
c. Differential (Q)PSK
4. Comparison of Modulation Formats in WDM Transmission
5. Conclusions
wr, APOC 2003; slide 4
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Modulation of a carrier signal (here: laser light) = mapping of
information into one or more parameters of the carrier, i.e
– Amplitude
– Phase (or frequency as ω=dφ/dt)
– Polarization
Carrier = real-valued band-pass signal (electrical field):
Modulation: Basics
( )( ) ( ) cos[ ( )] Re{ ( ) }Cj tj tCE t a t t t a t e e ωφω φ= + = ⋅
A(t): Complex Envelope
•carries information
•Determines modulation format
( )A t
wr, APOC 2003; slide 5
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Digital transmission of bits b with bit rate rb=1/Tb
M=2m bits collected à one complex symbol d(k), symbol rate rS=1/TS=rb/M
Modulation: Basics
( ) ( ) ( )R Id k d k jd k= +
Parallel/SerialMapping
Binary Bits M-ary Symbols
Complex symbols:
( )( ) ( ) ( ) ( ) j tR IA t A t jA t a t e φ= + =Complex envelope: ( ) ( )S
kd k h t kT= ⋅ −∑
Pulse shape
Transmitted field: ( ) ( ) ( ) cos( ) ( ) ( ) sin( )R S c I S ck k
E t d k h t kT t d k h t kT tω ω
= − − − ∑ ∑
Orthogonal carriers, 2 data streams
wr, APOC 2003; slide 6
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Linear Modulation: Constellations
In the class of linear modulationà format is determined by constellation
Noise performance à Minimum distance between symbols!
wr, APOC 2003; slide 7
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Modulation Formats: Some Options
• Amplitude – RZ/NRZ (2-ASK with different pulse shape)– VSB/SSB – Multilevel (4-ASK, 8-ASK)
• Phase– DPSK– DQPSK– CPM = continuous phase mod.
• Frequency– MSK = minimum shift keying– FSK = frequency shift keying
• Hybrid– CS-RZ, chirped RZ/NRZ, partial response (e.g.
duobinary)
wr, APOC 2003; slide 8
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Optical Modulator: Mach-Zehnder Interferometer
Mach-Zehnder Modulator for arbitraryphase/amplitude modulation
By driving and/or biasing a MZM apropriately, arbitrary constellations in complex plane can be implemented!
Ein,Pin Eout ,Pout
Wave-guide ∆φ1
∆φ2U2
U1
ok_32_modulator.dsf
wr, APOC 2003; slide 9
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Innovative Formats: Duobinary Signaling
• Reduced bandwidth (approx. Factor of 2 against NRZ)• Highly dispersion tolerantà increase uncompensated
transmission reach• Carrier suppressed format: relaxed SBS suppression
requirements • Increased spectral efficiency• Low implementation complexity à upgrade of conventional
IM/DD possible
wr, APOC 2003; slide 10
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Duobinary Signaling - How it Works!
• Optical transmitted signal: (pseudo)-three-level symbols {+1,0,-1}
using 2Vπ MZM drive signal• Coding rule:
– “0”-bit à 0– “1”-bit à +1 or –1, depending on depending on ……??
• Coding rule narrows spectrum of optical transmit signal• IM/DD-RX detects magnitude squared of opt. Signal
– 0-symbol à “0”-bit– +1-symbol and –1-symbol à “1”-bit
• Low implementation complexity – Implementation of coding rule in transmitter – Conventional IM/DD receiver– à simple upgrade of conventional IM/DD schemes
coding rule inverted!
wr, APOC 2003; slide 11
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Duobinary Signaling - Implementation
• Duobinary precoder = differential encoder à IC-solution• Duobinary filter: LP with cut-off frequency of fb/4
datagenerator
data
bias
duobinaryprecoding
MZMpush-pullCW laser
LPfilter three-level
data
clock&datarecovery
Duobinary Encoding
wr, APOC 2003; slide 12
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Duobinary Signaling - Dispersion Tolerance
• Improved dispersion tolerance• High sensitivity to non-linear fibre effects (SPM)
Simulation 10Gb/s Measurement 10Gb/s
wr, APOC 2003; slide 13
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Innovative Formats: SSB/VSB
• Single Side Band (SSB) or Vestigial Side Band (VSB)• Reduced bandwidth (approx. factor 2 against conventional
double-sideband ASK = DSB)• Highly dispersion tolerant• Increased spectral efficiency• Medium to high implementation complexity• Extinction ratio problems! à reduced receiver sensitivity
wr, APOC 2003; slide 14
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
SSB/VSB – How it Works!
• Conventional: Double side-band ASK• However: Redundancy à one side-band (either lower or
upper) is redundant (one SB contains full information!)• Eliminate one side-band by
– Filtering in optical domain– Filtering in electrical domain
• SSB/VSB RX requires coherent detection!• However direct (intensity) detection possible, but carrier
component required! • Direct detection results in distortions!
wr, APOC 2003; slide 15
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
SSB/VSB – Sideband Suppression
• Optical SSB/VSB filter• Filtering in optical
(band-pass) domain
• Hilbert Transformer = Phase response Filter
• Filtering in electrical (base-band) domain
USBLSB
HSSB(f)
fCfC+fofC+fu f
e.g. 60dB!
nu_9_ESB_AM.dsf
USBLSB
HH(f)
f=0fofu f
nu_9_ESB_AM.dsf
ideal
real
j
- j
wr, APOC 2003; slide 16
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
SSB/VSB – Implementation: Optical Filter
• Optical filtering of conventional IM (DSB) signal• Steep filter slope required• Approximation through sideband attenuation• Used for Tb/s-experiments by Alcatel
Pulse PatternGenerator
DataDataRF Bias
RF Amplifier
LaserMach -ZehnderModulator
VSB signaloptical Filter
wr, APOC 2003; slide 17
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
SSB/VSB – Implementation: Phase Method
• Phase inversion of one sideband in electrical base-band domain (Hartley)
• Hilbert transformer may be approximated by FIR (finite impulse response) filter
DataData
RF
Mach -ZehnderModulator
Laser
Puls PatternGenerator
RF Amplifier
π/2
coupler
Mach -ZehnderModulator
H
LT
TBiasRF
Bias
HilbertTransformator
optical SSB signal
RF Amplifier
Divider
wr, APOC 2003; slide 18
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
SSB/VSB – Implementation: Electrical Hilbert Transformer
Reduced complexity compatible SSB with electrical Hilbert Transformer
Phase-modulator
Pulse PatternGenerator
DataDataRF
optical SSB signal
HHilbertTransformer
Laser
RF Amplifier
RF Bias
Mach -ZehnderModulator
DSB
RF Amplifier
Bias
m(t) m(t)
Amplitude Modulation Phase Modulation
wr, APOC 2003; slide 19
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
SSB/VSB – Implementation: Electrical Hilbert Transformer 2
( ) ( )( ) cos exp
2 2bias
out inm t U m t
E t E jU Uπ π
π π −= ⋅ ⋅ ⋅
AM PM
m(t) - data signalm(t) - Hilbert transformed data signal
transfer function of SSB transmitter
+
( ) [ 1 ( ) ( ) ...]2 22
inout
EE t m t j m t
U Uπ π
π π≈ + ⋅ + ⋅ ⋅ +
Approximation for a linear driven MZ-modulator
=+j·m(t)m(t)1
SSB!
wr, APOC 2003; slide 20
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
SSB/VSB: Performance
• Method used: Electrical H.T. • Method requires approx. linear MZM drive conditions for
good side-band suppressionà Extinction ratio reduced!
Transfer characteristic of the Mach-Zehnder modulator for power P and electrical field E
Optical power spectral density (simulation)
0 +1
t
U
P
Et
0
+1P
-30 -20 -10 0 10 20 30-60
-50
-40
-30
-20
-10
0Power Spectral Density
Frequency [GHz]
PS
D [d
B] SSB
DSB
wr, APOC 2003; slide 21
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
SSB/VSB: Experimental comparison DB vs. SSB
• 200km uncompensated SSMF, 10Gb/s
• Compare SSB with duobinary
• Linear and non-linear fiber regime
• SSB approx. 6dB penalty, due to reduced extinction ratio 10-10
10-910-810-7
10-6
10-5
10-4
10-3
10-2
Bit
Err
or R
atio
(B
ER
)
receiver input power [dBm]-40 -38 -36 -34 -32 -30 -28 -26 -24 -22 -20
1.7dB
0.8dB
DB0dBm8dBm
SSB0dBm
8dBm
wr, APOC 2003; slide 22
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
SSB/VSB: Dispersion Tolerance DSB vs. SSB
• Simulation result, 10Gb/s
• Linear fiber• SSB: Extinction ratio
optimized for maximum reach
• DSB: maximum extinction ratio
0 50 100 150 200 250-2
0
2
4
6
8
10
12
14
SSMF length [km]
Eye
Ope
n P
enal
ty [d
B]
DSB
SSB
wr, APOC 2003; slide 23
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Binary Differential PSK (D-2-PSK)
• Symbols: +1, -1 • NRZ or RZ pulse shape possible
– RZ: +1,-1 identical optical intensity • à optical intensity = periodic function of time• à advantage in XPM environment
• Improved noise performance vs. conventional IM/DD , if balanced receiver used (3dB)
• Differential scheme à avoids coherent detection• Additional DPSK receiver (MZDI) necessary!• Differential precoder necessary!
wr, APOC 2003; slide 24
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Binary DPSK
• DPSK precoder = differential encoder (same as for duobinary)
• Functionality of MZDI receiver. Phase
cos( ( )) cos( ( 1))2
c ct k t kω φ ω α φ+ + − − +
{ }( ) 0,kφ π∈
[ ]{cos ( ) ( 1)0
k kφ φ α− − −=
64444744448... 2cos(...) cos(...) ...= + ⋅ +
( ) ( -1),( ) ( -1)
High if
Low if
k kk k
φ φφ φ
=≠
datagenerator
bias
dataclock
bias
RZ-pulse carving
PSKprecoding
CW laser
delay
Tb
clock&datarecovery
balancedreceiverdelay
interferometer
2VΠ-MZMpush-pull
wr, APOC 2003; slide 25
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Quaternary DPSK
• Our solution: serial DQPSK-transmitter à reduced complexity, relaxed phase control
• 2 parallel data streams (real & imaginary) with speed and bandwidth requirements of single data stream!
• Quaternary differential precoder required
datagenerator
bias
dataclock
bias bias
RZ-pulse carving
QPSKprecoding
MZMpush-pull
phasemodulator
S/P
CW laser
data real
data imag
delay interferometerwith carrier shift π/4
datarealdelay
Tb
balancedreceiver
π/4
dataimagdelay
Tbπ/4
wr, APOC 2003; slide 26
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
DPSK: Receiver Sensitivity - Theory
• Ideal coherent/synchronous detection: à both DPSK & DQPSK 3dB sensitivity improvement due to enlarged symbol distance (constellation!) vs. OOK=IM/DD!
• DPSK with MZDI = non-coherent: 0.2dB loss
• DQPSK with MZDI = non-coherent: 2dB loss
10 12 14 16 18
1e-5
1e-6
1e-7
1e-8
1e-9
1e-10
1e-11
Bit
Err
or R
atio
(B
ER
)
SNR [dBm]
DPSK
DQPSK
OOK
wr, APOC 2003; slide 27
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
DPSK with RZ pulse shape in WDM: Robustness towards XPM
• RZ: periodic optical intensity àsuppression of XPM-induced phase modulation
• RZ-DPSK extends transmission distance significantly!
Simulation result: 8x10Gb/s WDM, channel spacing: 100GHz,launch power: 9dBm/channelspan length: 100km SSMF, dispersion comp.
5 0 0 1 0 0 0 1 5 0 0 2 0 0 0 2 5 0 0 3 0 0 0- 0 . 5
0
0 . 5
1
1 . 5
2
2 . 5
3
L [km]E
OP[
dB]
RZ-ASK
RZ-DPSK
wr, APOC 2003; slide 28
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Modulation Formats in WDM Transmission
Power spectral density of various modulation formats at40Gb/s
-80 -60 -40 -20 0 20 40 60 80-50
-40
-30
-20
-10
0
10
20
f [GHz]
PS
D[d
B]
NRZ-ASK
SSB
DB RZ-DQPSK
40
SSB
70
NRZ-ASK
5648∆f [GHz]
RZ-DQPSKDB
Two-sided spectral width for a decay of 20dB for DB, SSB, RZ-DQPSK and NRZ-ASK at 40Gb/s
wr, APOC 2003; slide 29
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Modulation Formats and WDM: Intermodulation 0.8b/s/Hz
• Single channel: 4 spans 100km SSMF, Dispersion optimized, 40Gb/s
• RZ-DQPSK most robust against SPM and chrom. Dispersion!
0 1 2 3 4 5 6 7 80
1
2
3
4
5
average input power [dBm]
EO
P [
dB]
NRZ-AS K
SSB
DB
RZ-AS K
RZ-DQPSK
• WDM 8x40Gb/s, ∆f=50GHz: 4 spans 100km SSMF, Dispersion optimized
• RZ-DQPSK most robust against WDM intermodulation(XPM,FWM,SPM, linear cross-talk!)
0 1 2 3 4 5 6 7 80
1
2
3
4
5WDM 50GHz, dispersion optimized
Mean opt. Input power per channel [dBm]
eye
open
ing
pena
lty
[dB
]
RZ-DQPSK
DB
SSB NRZ-ASK100GHz
RZ-AS K 100GHz
wr, APOC 2003; slide 30
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Modulation Formats in WDM: Intermodulation
Sensitivity to nonlinear fibre effects, SSMF, 40Gb/s, ∆f=50GHz, 0.8b/s/Hz
0 1 2 3 4 5 6 7 8
0
1
2
3
4
5
average input power per ch. [dBm]
eye
open
ing
pena
lty
[dB
]
lin. Xtalk+all nonlinear.lin. Xtalk+SPM+XPMlin. Xtalk+SPM
0 1 2 3 4 5 6 7 8
0
1
2
3
4
5
average input power per ch. [dBm]
eye
open
ing
pena
tly
[dB
]lin. Xtalk+SPMlin. Xtalk+SPM+XPMlin. Xtalk+all nonlinear.
0 1 2 3 4 5 6 7 8
0
1
2
3
4
5
average input power per ch. [dBm]
eye
open
ing
pena
lty
[dB
]
lin. Xtalk+SPMlin. Xtalk+SPM+XPMlin. Xtalk+all nonlinear.
RZ-DQPSK
SSB
DB
FWMXPMSPMLinearcross-talk
wr, APOC 2003; slide 31
Chair forCommunications
Faculty of EngineeringChristian-Albrechts-University of Kiel
L N T
Conclusions
• Duobinary: low complexity, high benefit through spectral narrowing à
promising candidate for system upgrade now!
• SSB/VSB: solution with optical filtering à moderate system improvement
for reasonable additional complexity
• DPSK: medium complexity à high benefit through improved receiver
sensitivity and WDM intermodulation robustness
• DQPSK: medium to high complexity à but doubles channel capacity
• Other advanced formats: (MSK, CPM, M-PSK, M-QAM) worth investigating
in optical environment! à constraints: complexity and chirp!