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Investigation of Control Pulse Power Effects on Alloptical SMZ Switch Performance

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Terahertz Optical Asymmetric Demultiplexer (TOAD) Symmetric Mach-Zehnder (SMZ) ... TOAD: Closed loop with a nonlinear semiconductor optical amplifier (~mm) ... – PowerPoint PPT presentation

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Title: Investigation of Control Pulse Power Effects on Alloptical SMZ Switch Performance


1
Investigation of Control Pulse Power Effects on
All-optical SMZ Switch Performance
  • H. Le Minh, Z. Ghassemlooy and Wai Pang Ng
  • Optical Communications Research Group
  • Northumbria University, UK
  • http//soe.unn.ac.uk/ocr/

5th International Symposium on Communication
Systems, Networks and Digital Signal Processing
(CSNDSP 2006) Patras (Greece), 19th - 21st July
2006
2
Contents
  • Introduction
  • Overviews of All-optical Switches
  • Numerical modelling of SMZ with unequal
    control-pulse powers
  • SMZ switch
  • Residual Crosstalk Issue
  • Unequal control-pulse power scheme
  • Simulation results
  • Summary

3
Introduction All-optical network
  • Network transparency ? All-optical core router
  • Processing, switching and routing in optical
    domain ? high aggregate throughput
  • Optical data packet format is preserved
  • Low BER (w/o FEC) and low power penalty of
    switching/routing at each router

1
4
All-optical Switching
1?2
Control path
Case I Without control signals (non-switching
mode) a) Packets are switched to
lower output port b) No signals at
the upper output port (i.e. High
switching extinction ratio)
2
5
All-optical Switching (cont.)
1?2
Control path
  • Electrical Switching
  • Optical packets have to be converted to
    electrical domain
  • Electronically switching speed limitation (lt 40
    Gbits/s)
  • All-optical Switching
  • Packets remain in optical domain (no error
    addition)
  • Ultrafast switching/demultiplexing (up to 160
    Gbits/s)

Case II With control signals (switching mode)
a) Packets are switched to upper
output port b) Control signals set
the ON/OFF of the output ports
2
6
All-optical Switching (cont.)
  • Ultrafast all-optical switches (gt 80 Gbits/s) are
    based on
  • Optical interferometer Nonlinear Element
  • Proposed optical switch configurations
  • Nonlinear Optical Loop Mirror (NOLM)
  • Terahertz Optical Asymmetric Demultiplexer (TOAD)
  • Symmetric Mach-Zehnder (SMZ)
  • Ultrafast Nonlinear Interferometer (UNI)

3
7
All-optical Switching (cont.)
  • Ultrafast all-optical switches (gt 80 Gbits/s) are
    based on
  • Optical interferometer Nonlinear Element
  • Proposed optical switch configurations
  • Nonlinear Optical Loop Mirror (NOLM)
  • Terahertz Optical Asymmetric Demultiplexer (TOAD)
  • Symmetric Mach-Zehnder (SMZ)
  • Ultrafast Nonlinear Interferometer (UNI)

NOLM Closed loop with a long strong nonlinear
fiber loop (km) Complex and
consuming high optical energy
3
8
All-optical Switching (cont.)
  • Ultrafast all-optical switches (gt 80 Gbits/s) are
    based on
  • Optical interferometer Nonlinear Element
  • Proposed optical switch configurations
  • Nonlinear Optical Loop Mirror (NOLM)
  • Terahertz Optical Asymmetric Demultiplexer (TOAD)
  • Symmetric Mach-Zehnder (SMZ)
  • Ultrafast Nonlinear Interferometer (UNI)

TOAD Closed loop with a nonlinear semiconductor
optical amplifier (mm) Complex
but consuming less optical energy
3
9
All-optical Switching (cont.)
  • Ultrafast all-optical switches (gt 80 Gbits/s) are
    based on
  • Optical interferometer Nonlinear Element
  • Proposed optical switch configurations
  • Nonlinear Optical Loop Mirror (NOLM)
  • Terahertz Optical Asymmetric Demultiplexer (TOAD)
  • Symmetric Mach-Zehnder (SMZ)
  • Ultrafast Nonlinear Interferometer (UNI)

SMZ Short two-waveguide-arms loop with two
identical SOA (mm) Compact
(integration capability) and consuming much less
optical energy
3
10
All-optical Switching (cont.)
  • Ultrafast all-optical switches (gt 80 Gbits/s) are
    based on
  • Optical interferometer Nonlinear Element
  • Proposed optical switch configurations
  • Nonlinear Optical Loop Mirror (NOLM)
  • Terahertz Optical Asymmetric Demultiplexer (TOAD)
  • Symmetric Mach-Zehnder (SMZ)
  • Ultrafast Nonlinear Interferometer (UNI)

UNI Long briefinger fibre with a SOA (mm)
Polarization-dependence issue, consuming low
optical energy as SMZ
3
11
All-optical SMZ Switch
Switching mode a) 2?2 (3-dB)
couplers and optical waveguides
form the constructive/destructive
interferometer b) CP1 and CP2 control
the SOA1 and SOA2 nonlinearities
to change the input signal gain/phase ? Switching
4
12
All-optical SMZ Switch (cont.)
Gain profile of the SOA
(1)
6
13
All-optical SMZ Switch (cont.)
Switching window (SW) gain
(2)
SW width Delay interval between two control
pulses TSW
7
14
Residual Crosstalk in SMZ
SOA recovery region
Switching window
SOA gains
Residual gain Owing to the difference of SOA
gains in recovery region, SW(t) is non zero
outside TSW
8
15
Residual Crosstalk in SMZ (cont.)
Residual Crosstalk
(3)
  • Pnt the sum of the output signal power of all
    non-target channels
  • Pt the output signal power of the target channel

9
16
Unequal Control-pulse power scheme
a) Equal CPs scheme
b) Unequal CPs scheme
Suppress CXT by overlapping G1 and G2 in gain
recovery region ? PCP1 gt PCP2
? Solving these equations
(4)
R power reduction ratio
10
17
Unequal Control-pulse power scheme (cont.)
Finding the optimum R
Solving (4) to obtain the reduction ratio R
between PCP1 and PCP2
Crosstalk is dependent on the injected CP power
(PCP1) and the reduction ratio R SOA
simulation parameters given in Table 1 in Result
Section
11
18
Simulation Parameters
Table 1 Main parameters
12
19
Simulation Results
Case I Demultiplexing 160-to-10 Gbit/s
Demultiplexing with equal CPs
Demultiplexing with unequal CPs
BER and Power penalty are improved 1dB
13
20
Simulation Results (cont.)
Case I Demultiplexing 160-to-10 Gbit/s
Received power penalty vs. different
demultiplexed OTDM channels (at BER 10-9)
Received power penalty vs. the control power of
PCP1 at R 0 dB and at Ropt
  • Power penalty variation among demultiplexed
    channels is small
  • Improvement of 1 dB achieved by using optimum
    Ropt

14
21
Simulation Results (cont.)
Case II Demultiplexing at high demltiplexing
rate (160-to-80/160-to-40/160-to-20 Gbit/s)
Improvement
Ropt offers significant reduced power penalty at
high demultiplexing rates
Received power penalties vs. different
demultiplexing rates from an OTDM bit stream of
160 Gb/s
15
22
Simulation Results (cont.)
Case III Switching with wide SW (TSW gt one
channel) and short switching interval (Tint)
Non-overlapping gain recovery region
Overlapping gain recovery region
Switching Extinction ratio (r) is much improved
TSW 4 channels
a) Equal CPs scheme
b) Unequal CPs scheme
16
23
Simulation Results (cont.)
Case III Switching with wide SW (TSW gt one
channel) and short switching interval (Tint)
Unequal CPs r is achieved gt 30 dB
Equal CPs r is small (lt 20 dB)
The extinction ratio (r) vs. the switching
interval (Tint) for various switching window
widths (TSW), at Ropt, and with the bit stream of
160 Gbit/s
17
24
Summary
  • Unequal control-pulse power scheme
  • Suppression the residual crosstalk by setting
    reduction ratio between control pulses
  • BER and received power penalty of SMZ-based
    demultiplexer are reduced in 1 dB
  • Switching extinction ratio is enhanced by more
    than 10-dB
  • The scheme is effective and simple to implement

18
25
Acknowledgement
Northumbria University for supports and
sponsoring this research
26
Thank you.
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