Transcript Optical Wireless Communication using Digital Pulse
Free Space Optical Communications
Professor Z GHASSEMLOOY
Associate Dean for Research
Optical Communications Research Group, School of Computing, Engineering and Information Sciences The University of Northumbria Newcastle, U.K.
http://soe.unn.ac.uk/ocr/ Iran 2008 1
Northumbria University at Newcastle, UK
2 2 Iran 2008
Outline
Introduction Why the need for optical wireless?
FSO FSO - Issues Some results Final remarks
3 Iran 2008 3
OCRG -
Research Areas
Optical Communications
Wired Wireless Optical Fibre Communications • • • •
Chromatic dispersion compensation using optical signal processing Pulse Modulations Optical buffers Optical CDMA
Photonic Switching • •
Fast switches All optical routers
Indoor • • • •
Pulse Modulations Equalisation Error control coding Artificial neural network & Wavelet based receivers Free-Space Optics (FSO)
Subcarrier modulation Spatial diversity
Artificial neural network/Wavelet based receivers
4 HK Poly-Univ. 2007
OCRG People
Staff
• Prof. Z Ghassemlooy • J Allen • R Binns • K Busawon • Wai Pang Ng •
Visiting Academics
Prof. Jean Pierre, Barbot
France
• Prof. I. Darwazeh
UCL
• Prof. Heinz Döring
Hochschule Mittweida Univ. of Applied Scie. (Germany)
• Dr. E. Leitgeb
Graz Univ. of Techn. (Austria)
PhD
• M. Amiri • M. F. Chiang: • S. K. Hashemi • R. Kharel • W. Loedhammacakra • V. Nwanafio • E. K. Ogah • W. O. Popoola • S. Rajbhandari (With IMLab) • Shalaby • S. Y Lebbe • • • •
MSc and BEng
A Burton • D Bell G Aggarwal • M Ljaz O Anozie • W Leong (BEng) S Satkunam (BEng)
Photonics Applications
• Photonics in communications: expanding and scaling 6 Long-Haul Metropolitan Home access Board -> Inter-Chip -> Intra-Chip • Photonics: diffusing into other application sectors Health (“bio-photonics”) Environment sensing Security imaging Iran 2008
RF & Optical Communications Integration
Radio on Fibre Traditional Radio Traditional Optics Optical Wireless
Fibre Free Space Transmission Channel
Free Space Optical (FSO) Communications
The Problem?
AND THAT IS ?
….. BANDWIDTH when and where required.
Over the last 20 years deployment of optical fibre cables in the backbone and metro networks have made huge bandwidth readily available to within one mile of businesses/home in most places.
But
, HUGE BANDWIDTH IS STILL NOT AVAILABLE TO THE END USERS.
9
10
Optical Wireless Communication
Abundance of unregulated bandwidth -
200 THz in the 700-1500 nm range
No multipath fading -
Intensity modulation and direct detection
What does It Offer ?
High data rate –
In particular line of sight (in and out doors)
Improved wavelength reuse capability Flexibility in installation Secure transmission Flexibility -
Deployment in a wide variety of network architectures. Installation on roof to roof, window to window, window to roof or wall to wall.
Iran 2008 10
11
Optical Wireless Communication
D r a w b a c k s
Multipath induced dispersion (non-line of sight, indoor) -
Limiting data rate
SNR can vary significantly with the distance and the ambient noise (Note SNR
P r
2 ) Limited transmitted power -
Eye safety (indoor)
High transmitted power -
Outdoor
Receiver sensitivity May be high cost -
Compared with RF
Large area photo-detectors -
Limits the bandwidth
Limited range:
Indoor:
ambient noise is the dominant (20-30 dB larger than the signal level
. Outdoor:
Fog and other factors
11 Iran 2008
Access Network bottleneck
12 12 12 (Source: NTT) Iran 2008
Access Network Technology
xDSL
Copper based (limited bandwidth)- Phone and data combine Availability, quality and data rate depend on proximity to service provider’s C.O.
Radio link
Spectrum congestion (license needed to reduce interference) Security worries (Encryption?) Lower bandwidth than optical bandwidth At higher frequency where very high data rate are possible, atmospheric attenuation(rain)/absorption(Oxygen gas) limits link to ~1km
Cable
Shared network resulting in quality and security issues.
Low data rate during peak times
FTTx
Expensive Right of way required - time consuming Might contain copper still etc 13 Iran 2008 13
Optical Wireless Communications
Using optical radiation to communicate between two points through unguided channels
Types
- Indoor
- Outdoor (Free Space Optics)
14 Iran 2008 14
FSO Basics
Cloud Rain Smoke Gases Temperature variations Fog and aerosol
Transmission of optical radiation through the atmosphere obeys the Beer Lamberts’s law: 2
P r
P t
d
1 2 (
D
2
L
) 2 10
L
/ 10 Dominant term at 99.9% availability α
:
Attenuation coefficient dB/km –
Not controllable and is roughly independent of wavelength in heavy attenuation conditions.
d
1 and
d
2 : Transmit and receive aperture diameters (m)
D: B
eam divergence (mrad)(1/
e
for Gaussian beams; FWHA for flat top beams), This equation fundamentally ties FSO to the atmospheric weather conditions Link Range L 15
FSO Link
Transmitter
Lasers 780,850,980,1550nm, also 10 microns Beam control optics o Multiple transmit apertures to reduce scintillation problems o Tracking systems to allow narrow beams and reduced geometric losses
Receiver
Collection lens Solar radiation filters (often several) Photodetector Large area and low capacitance (PIN/APD) Amplifier and receiver o Wide dynamic range requirement due to very high clear air link margin o Automatic gain and transmitter power control
Optical Components – Light Source
Operating Wavelength (nm)
~850 ~1300/~1550
Laser type Remark
VCSEL Fabry-Perot/DFB Cheap, very available, no active cooling, reliable up to ~10Gbps, Long life, compatible with EDFA, up to 40Gbps 50 –65 times as much power compared with 780-850 nm ~10,000 Quantum cascade laser (QCL) Expensive, very fast and highly sensitive Ideal for indoor (no penetration through window)
For indoor applications LEDs are also used
Eye safety -
17 Class 1M Iran 2008 17
Optical Components – Detectors
Material/Structure Silicon PIN InGaAs PIN Silicon APD Wavelength (nm)
300 1000 400 – 1100 – 1700 – 1000
Responsivity (A/W) Typical sensitivity
0.5
0.9
-34dBm@ 155Mbps -46dBm@ 155Mbps 77 -52dBm@ 155Mbps 9
Gain
1 1 150
InGaAs APD Quantum –well and Quatum-dot (QWIP&QWIP)
1000 – 1700 ~10,000 10
Germanium only detectors are generally not used in FSO because of their high dark current.
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Existing System Specifications
Range: 1-10 km (depend on the data rates) Power consumption up to 60 W 15 W @ data rate up to 100 mbps and 25 W @ date rate up to 150 Mbps and =780nm, short range = 980nm 60 W @ data rate up to 622 Mbps and 40 W @ data rate up to 1.5 Gbps and = 780nm = 780nm Transmitted power: 14 – 20 dBm Receiver: PIN (lower data rate), APD (>150 mbps) Beam width: 4-8 mRad Interface: coaxial cable, MM Fibre, SM Fibre Safety Classifications: Class 1 M (IEC) Weight: up to 10 kg 19
Power Spectra of Ambient Light Sources
1.2
1 0.8
0.6
0.4
0.2
0
P ave)amb-light >> P ave)signal (Typically 30 dB with no optical filtering) Sun Incandescent
1 st window IR
Fluorescent
x 10 2 nd window IR 20 20 Wavelength ( m) Iran 2008
FSO Characteristics
Narrow low power transmit beam inherent security Narrow field-of-view receiver Similar bandwidth/data rate as optical fibre No multi-path induced distortion in LOS Efficient optical noise rejection and a high optical signal gain Suitable to point-to-point communications only (out-door and in-door) Can support mobile users using steering and tracking capabilities Used in the following protocols: - Ethernet, Fast Ethernet, Gigabit Ethernet, FDDI, ATM - Optical Carriers (OC)-3, 12, 24, and 48. Cheap (cost about $4/Mbps/Month according to fSONA) 21 Iran 2008 21
Cost Comparison
22 Source: 22 Iran 2008
Existing Systems
Auto tracking systems - 622 Mbps [Canobeam] TereScop - 1.5 Mbps to 1.25 Gbps (500m – 5km) Cable Free - 622 Mbps to 1.25 Gbps (High power class 3B Laser at 100 mW) Microcell and cell-site backbone – GSM, GPRS, 3G and EDGE traffic o No Frequency license o No Link Engineering o Management via SNMP, RS232 o or GSM connection Last mile o 155 Mbps STM-1 links o 622 Mbps ATM link for Banks etc
When Did It All Start?
800BC - Fire beacons (ancient Greeks and Romans) 150BC - Smoke signals (American Indians) 1791/92 - Semaphore (French) 1880 Alexander Graham Bell demonstrated the photophone –
FSO (
THE GENESIS)
1 st
24 (www.scienceclarified.com) 1960s - Invention of laser and optical fibre 1970s - FSO mainly used in secure military applications 1990s to date - Increased research & commercial use due to successful trials 24 Iran 2008
FSO Applications
In addition to bringing huge bandwidth to businesses /homes FSO also finds applications in : 25
Hospitals Cellular communication back-haul Others:
Inter-satellite communication
Disaster recovery
Fibre communication back-up
Video conferencing
Links in difficult terrains
Temporary links Multi-campus university e.g. conferences
25
FSO challenges…
Iran 2008
Hybrid FSO/RF Wireless Networks
RF wireless networks
Broadcast RF networks are not scaleable RF cannot provide very high data rates RF is not physically secure - High probability of detection/intercept Not badly affected by fog and snow, affected by rain
A Hybrid FSO/RF Link
- High availability (>99.99%) - Much higher throughput than RF alone - For greatest flexibility need unlicensed RF band
LOS Hybrid Systems
27 Video-conference for Tele-medicine CIMIC-purpose and disaster recovery 27 Iran 2008
FSO Challenges
Major challenges are due to the effects of: CLOUD, RAIN, SMOKE, GASES, TEMPERATURE VARIATIONS FOG & AEROSOL
POINT A To achieve optimal link performance, system design involves tradeoffs of the different parameters.
28 POINT B Iran 2008 28
FSO Challenges - Rain
= 0.5 – 3 mm
Effects
Photon absorption
Options Remarks
Increase transmit optical power Effect not significant 29 Iran 2008 29
FSO Challenges Physical Obstructions Pointing Stability and Swaying Buildings
Effects Solutions
Loss of signal Spatial diversity Multipath induced Mesh architectures: using Distortions Low power due to beam divergence and spreading diverse routes Ring topology: User ’ s n/w become nodes at least one hop away from the ring Fixed tracking (short Short term loss of buildings) signal Active tracking (tall buildings) 30
Remarks
May be used for urban areas, campus etc.
Low data rate Uses feedback
FSO Challenges
–
Aerosols Gases & Smoke
Effects
Mie scattering Photon absorption Rayleigh scattering
Solutions
Increase transmit power Diversity techniques
Remarks
Effect not severe 31
FSO Challenges - Fog
= 0.01 - 0.05 mm In heavy fog conditions, attenuation is almost constant with wavelength over the 780 –1600 nm region.
In fact, there are no benefits until one gets to millimeter-wave wavelengths.
32
Effects
Mie scattering Photon absorption
Options
Increase transmit optical power Hybrid FSO/RF
Remarks
Thick fog limits link range to ~500m Safety requirements limit maximum optical power 32 Iran 2008
FSO Challenges - Fog
Weather condition Dense fog Thick fog Moderate fog Light fog Thin fog Haze Light haze Clear Very clear Precipitation Snow Snow Snow t Cloudburs Heavy rain Snow Snow Snow Medium rain Light rain Drizzle Amount (mm/hr) Visibility dB Loss/km Typical Deployment Range (Laser link ~20dB margin) 100 25 12.5
2.5
0.25
0 m 50 m 200 m 500 m 770 m 1 km 1.9 km 2 km 2.8 km 4 km 5.9 km 10 km 18.1 km 20 km 23 km 50 km -271.65
-59.57
-20.99
-12.65
-9.26
-4.22
-3.96
-2.58
-1.62
-0.96
-0.44
-0.24
-0.22
-0.19
-0.06
122 m 490 m 1087 m 1565 m 1493 m 3238 m 3369 m 4331 m 5566 m 7146 m 9670 m 11468 m 11743 m 12112 m 13771 m
33 (H.Willebrand & B.S. Ghuman, 2002.) Iran 2008 33
FSO Challenges Beam Divergence
Beam width Typically, for FSO transceiver is relatively wide: 2 –10-mrad divergence, (equivalent to a beam spread of 2 –10 m at 1 km), as is generally the case in non-tracking applications.
Compensation is required for any platform motion By having a beam width and total FOV that is larger than either transceiver’s anticipated platform motion. For automatic pointing and tracking, Beam width can be narrowed significantly (typically, 0.05
–1.0 mrad of divergence (equivalent to a beam spread of 5 cm to 1 m at 1 km) - further improving link margin to combat adverse weather conditions.
- However, the cost for the additional tracking feature can be significant.
FSO Challenges - Others
Background radiation LOS requirement Laser safety
35 Iran 2008
Free Space Optics
Characteristics
Challenges Turbulence - Subcarrier intensity multiplexing - Diversity schemes
Results and discussions
Wavelet ANN Receiver
Final remarks
FSO Challenges Turbulence
Effects Options
Irradiance fluctuation
Diversity techniques (scintillation)
Forward error control
Image dancing Phase fluctuation
control
Robust modulation
Beam spreading
techniques
Polarisation fluctuation Adaptive optics Coherent detection not used due to Phase fluctuation 37
Remarks
Significant for long link range (>1km) Turbulence and thick fog do not occur together In IM/DD, it results in deep irradiance fades that could last up to ~1 100 μs
FSO Challenges - Turbulence
Cause: path.
Atmospheric inhomogeneity / random temperature variation along beam The atmosphere behaves like prism of different sizes and refractive indices
38
Phase and irradiance fluctuation
Result in deep signal fades that • Zones of differing density act as lenses, lasts for ~1 100 μs scattering light away from its intended path. • Thus,
multipath
.
Depends on:
Altitude/Pressure, Wind speed,
Temperature and relative beam size.
Can change by more than an order of magnitude during the course of a day, being the worst, or most scintillated, during midday (highest temperature).
However, at ranges < 1 km, most FSO systems have enough dynamic range or margin to compensate for scintillation effects.
Iran 2008
39
Turbulence – Channel Models
Irradiance PDF:
p I
(
I
) 1 2
l
1 exp
I
(ln(
I
/
I
0 ) 2
l
2
l
2 / 2 ) 2
I
0
Model
Log Normal I-K K Rayleigh/Negative Exponential Gamma-Gamma
Comments
Simple; tractable Weak regime only Weak to strong turbulence regime Strong regime only Saturation regime only All regimes Irradiance PDF by Andrews et al (2001): Based on the modulation process the received irradiance is
I
I x y p
(
I
) 2 ( ( ) ( ) ) ( ) / 2
I
( 2 ) 1 ( 2
I
)
I
0 I x : due to large scale effects; obeys
Gamma distribution
exp ( 1 0 .
49
l
2 1 .
11
l
12 / 5 ) 7 / 6 exp ( 1 0 .
0 .
51
l
69
l
12 2 / 5 ) 5 / 6 1 1 1 1 To mitigate turbulence effect we, employ subcarrier modulation with spatial diversity I y : due to small scale effects; obeys Gamma distribution K
n
(.): modified Bessel function of the 2nd kind of order
n
σ
l
2 : Log irradiance variance (turbulence strength indicator) Iran 2008
Turbulence Effect on OOK
No Pulse Bit “0” No Intensity Fading Threshold level A/2 With Intensity Fading A Pulse Bit “1” A
All commercially available systems use OOK with fixed threshold which results in sub-optimal performance in turbulence regimes
40 Iran 2008 40
Turbulence Effect on OOK
Using optimal maximum a posteriori (MAP) symbol-by-symbol detection with equiprobable OOK data:
d
ˆ (
t
) arg max
d P
(
i r
/
d
(
t
)) 0 exp exp ((
i r
ln(
I
RI
) 2
i r
2 ) 2 2 /
I
0 ) 2
l
2
l
2 / 2 2
dI
1 2
l
2 1 .
I
0.5
0.45
0.4
Noise variance 0.5*10 -2 10 -2 3*10 -2 5*10 -2 0.35
0.3
OOK based FSO requires adaptive threshold to perform optimally….
0.25
0.2
….but subcarrier intensity modulated FSO does not
0.15
0.1
0 0.1
0.2
0.3
0.4
0.5
0.6
0.7
Log Intensity Standard Deviation
0.8
0.9
41 1
SIM – System Block Diagram
d
(
t
) Data in Serial/parallel converter .
.
Subcarrier modulator DC bias
m
(
t
) .
.
Summing circuit
m
(
t
)+
b o
Optical transmitter Atmospheric channel
d
’(
t
) Data out Parallel/serial converter .
.
Subcarrier demodulator Spatial diversity combiner
i r
Photo detector array 42
Subcarrier Intensity Modulation
No need for adaptive threshold To reduce scintillation effects on SIM Convolutional coding with hard-decision Viterbi decoding (J. P. KIm et al 1997) Turbo code with the maximum-likelihood decoding (T. Ohtsuki, 2002) Low density parity check (for burst-error medium): - Outperform the Turbo-product codes. - LDPC coded SIM in atmospheric turbulence is reported to achieve a coding gain >20 dB compared with similarly coded OOK (I. B. Djordjevic, et al 2007) SIM with space-time block code with coherent and differential detection (H. Yamamoto, et al 2003) However, error control coding introduces huge processing delays and efficiency degradation (E. J. Lee et al, 2004) 43
SIM – Our Contributions
Multiple-input-multiple-output (MIMO)
photodetectors) to mitigate scintillation effect in a IM/DD FSO link overcomes
temporary link blockage
(an array of transmitters/ (birds and misalignment) when combined with a wide laser beamwidth, therefore no need for an active tracking provides
independent aperture averaging
aperture system, than in a single aperture where the aperture size has to be far greater than the irradiance spatial coherence distance (few centimetres) with multiple separate provides gain and bit-error performance Efficient
coherent modulation
techniques (BPSK etc.) - bulk of the signal processing is done in RF that suffers less from scintillation In dense fog, MIMO performance drops, therefore alternative configuration such as
hybrid FSO/RF
should be considered Average transmit power increases with the number of subcarriers, thus may suffers from signal clipping Inter-modulation distortion
45
Subcarrier Modulation Transmitter
A 1 g
(
t
) PSK modulator at cosw c1 t Input data
d
(
t
) Serial to Parallel Converter .
.
A 2
.
.
.
.
A M g
(
t
) PSK modulator at cosw c2 t
m
(
t
)
j M
1
A j g
(
t
) cos(
w cj t
j
)
Σ
m
(
t
)
Σ
Laser driver Atmopsheric channel DC bias
b 0 g
(
t
) PSK modulator at cosw cM t Modulation index is constrained to avoid over modulation 45 [
Rh
0
P t
, 0 0
N c
' ] 1 Iran 2008
46 1 2
Subcarrier Modulation Transmitter
0 -1 -2
m
(
t
)
j M
1
A j g
(
t
) cos(
w cj t
j
) 5-subcarriers -3 -4 -5 0 0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1 Output power
P
P
max 2 [
Rh
0
P t
, 0 0
N c
' ] 1 m(t)
b 0
Drive current Iran 2008
SIM Receiver
SNR ele
(
IRA
) 2 2 2
x
g(-t) PSK Demodulator Sampler
P r
i N
c
1
h i P t
,
i
1
d i
(
t
) cos( 2
f i t
cosw c1 t
n
(
t
) Photodetector PSK Demodulator at cosw c2 t
i r
.
.
.
Photo-current
PSK Demodulator at cosw cM t
i r
(
t
)
R
R I
( 1
m
(
t
))
n
(
t
) = Responsivity,
I
= Average power, = Modulation index,
m
(
t
) = Subcarrier signal di(
t
) = Data 47 Parallel to Serial Converter
d
ˆ (
t
) Output data
Subcarrier Modulation
Performs optimally without adaptive threshold as in OOK Use of efficient coherent modulation techniques (PSK, QAM etc.) - bulk of the signal processing is done in RF where matured devices like stable, low phase noise oscillators and selective filters are readily available.
System capacity/throughput can be increased Outperforms OOK in atmospheric turbulence Eliminates the use of equalisers in dispersive channels Similar schemes already in use on existing networks
But..
The average transmit power increases as the number of subcarrier increases or suffers from signal clipping.
Intermodulation distortion due to multiple subcarrier impairs its performance 48 Iran 2008 48
SIM Spatial Diversity
Single-input-multiple-output Multiple-input-multiple-output (MIMO)
49
F S O C H A N N E L
SIM Spatial Diversity
i
1 (
t
) a 1
i
2 (
t
)
i N
(
t
) a 2 .
.
.
a N .
Combiner Assuming identical PIN photodetector on each links, the photocurrent on each link is
:
i T
(
t
)
i ri
(
t
) PSK Subcarrier Demodulator
d
ˆ (
t
)
R N I i
1
M
j A j g
(
t
) cos(
w cj t
j
)
n i
(
t
)
a i
is the scaling factor
Maximum Ratio Combining (MRC)
a i i i
Diversity Combining Techniques
a
1 Equal Gain Combining (EGC)
a
2 ...
a N
Selection Combining (SELC). No need for phase information
i T
(
t
) max(
i
1 (
t
),
i
2 (
t
)...
i N
(
t
)) 50
SIM Spatial Diversity
–
Assumptions Made
Spacing between detectors > the transverse correlation size ρ o of the laser radiation, because ρ o = a few cm in atmospheric turbulence Beamwidth at the receiver end is sufficiently broad to cover the entire field of view of all
N
detectors. Scintillation being a random phenomenon that changes with time makes the received signal intensity time variant with coherence time o of the order of milliseconds. Symbol duration
T
<< o , thus received irradiance is time invariant over one symbol duration.
51
Subcarrier Modulation Spatial Diversity
52 One detector Two detectors Three detectors A typical reduction in intensity fluctuation with spatial diversity Eric Korevaar et. al Iran 2008
Free Space Optics
Characteristics
Challenges Turbulence - Subcarrier intensity multiplexing - Diversity schemes
Results and discussions
Wavelet ANN Receiver
Final remarks
Error Performance – No Spatial Diversity
Normalised SNR at BER of 10 -6 against the number of subcarriers for various turbulence levels for BPSK
20 15 10 5 Increasing the number of subcarrier/users, results In increased SNR 0 -5 -10 1 2 3 4 5 6
Number of subcarrier
7 8 Log intensity variance 0.1
0.2
0.5
0.7
9 10 SNR gain compared with OOK
Error Performance – No Spatial Diversity
55
BPSK BER against SNR for M-ary-PSK for log intensity variance = 0.5
2
10 -2 10 -4 DPSK BPSK 16-PSK 8-PSK Log intensity variance = 0.5
2 BPSK based subcarrier modulation is the most power efficient 10 -6 10 -8
BER
2 log 2
M
0
Q
SNR e
log 2
M
sin( /
M
)
p
(
I
)
dI
10 -10 20 25 SNR (dB) 30 35 40 Iran 2008
Spatial Diversity Gain
Spatial diversity gain with EGC against Turbulence regime
Saturation
70 60 50 40 30 20 10
Weak
2 Photodetectors 3 Photodetectors
Moderate Turbulence Regime
Iran 2008 56
Spatial Diversity Gain for EGC and SeLC
25 20 15 Log Intensity Variance 0.2
2 0.5
2 0.7
2 1 Link margin for SelC is lower than EGC by ~1 to ~6 dB 10 5 0 Dominated by received irradiance, reduced by factor
N
on each link.
-5 -10 1 EGC Sel.C
BER = 10 -6
2 3
P e
(
SelC
) 2
N N
4 5 6 7 8 9
i n
1 [
w i
No of Receivers
1
erf
(
x i
)
N
1 .
e
(
K
0 2 exp( 2
x i
i i n
= Zeros of the 1
n
th order Hermite polynomial 10 2
l
l
2 )) ]
n
= Weight factor of the
n
th order
i
1 Hermite polynomial
K
0
RI
0
A
2 2
N
Spatial Diversity Gain for EGC and MRC
30
BER = 10 -6
25 Log Intensity variance 1
P e
(
EGC
) 0 / 0 2 exp 2
K
1 2 sin 2 ( )
Z
2 1
m
1
w i Q
(
K
1
e
(
x i
2
u
u
) )
P Z
(
Z
)
d
dZ
20 MRC EGC 15 10 5 0.5
2 0.2
2
P e
(
MRC
) 1 0
Q
MRC
/
I
P I
(
I
)
d I
0 / 2
S
( )
N d
, 0 1 2 3
Most diversity gain region
4 5 6
No of Receivers
7 8 9 10
The optimal but complex MRC diversity is marginally superior to the practical EGC
58
Multiple-Input-Multiple-Output
I t1 d
(
t
)
I t2
BPSK Modu Lator and Laser driver
I tH
.
.
.
F S O C H A N N E L
i
1 (
t
) a 1 Combiner
i
2 (
t
)
i N
(
t
) a 2 .
.
.
.
a N
i T
BPSK Subcarrier Demodulator
d
ˆ (
t
) By linearly combining the photocurrents using MRC, the individual
SNRe
on each link
SNR ele
i
RA
2
N
2 59
H j H
1
I ij
2
MIMO Performance
10 -3 10 -4 10 -5 10 -6 10 -7 10 -8 10 -9 log intensity variance= 0.5
2 1X5MIMO 1X8MIMO 4X4MIMO 2X2MIMO 1X4MIMO
At BER of 10 -6 :
2 x 2-MIMO requires additional ~0.5 dB of SNR compared with 4 photodetector single transmitter multiple photodetector system.
4 x 4-MIMO requires ~3 dB and ~0.8 dB lower SNR compared with single transmitter with 4 and 8 photodetectors , respectively.
26
P e
12 1 14 16 18 20 22
SNR (R*E[I]) 2 / No (dB)
/ 0 2
S
( )
N d
, 24
S
( ) 1
j m
1
w j
exp 60
K
2
K
2 2 2 sin 2 exp[ 2 (
x j RI
0
A
2
N
2
H
2
u
u
)]
Free Space Optics
Characteristics
Challenges Turbulence - Subcarrier intensity multiplexing - Diversity schemes
Results and discussions Wavelet ANN Receiver
Final remarks
Transmission System Models Receiver
Data in TX Channel
+
Noise Data out
…
Slicer MMSE Data out Slicer Equaliser MF Data out Slicer Wavelet - NN NN CWT
Iran 2008 62
PPM System – NN Equalization
n
(
t
)
M
0 1 0 0 PPM Encoder
X j
Optical Transmitter
X
(
t
)
h
(
t
) ∑
Z(t )
Optical Receiver
M
0 0 1 0 PPM Decoder Decision Device
Y j
Neural Network .
Z j Z j
-1 .
Z j
-
n Z j T s = M
/
LR b
Matched Filter A feedforward back propagation neural network .
ANN is trained using a training sequence at the operating SNR.
Trained AAN is used for equalization 63 Iran 2008
Impulse Response of Equalized Channel
64 Impulse response of unequalized channel impulse response of equalized channel • Pulse are spread to adjust pulse . • ISI depends on pulse spread • Equalized response in a delta function which is equivalent to a impulse response of the ideal channel Iran 2008
Results (1)
Slot error rate performance of 8- PPM in diffuse channel with D rms Mbps of 5ns at 50 65 Adaptive linear equalizer with least mean square (LMS) algorithm is used.
The performance of ANN equalizer is almost identical to the linear equalizer.
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Results (2)
Slot error rate performance of 8- PPM in diffuse channel with D rms Mbps of 5ns at 100 66 Unequalized performance at higher data rate is unacceptable at all SNR range Linear and neural equalization give almost identical performance.
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Results (3) Wavelet-AI Receiver
67 Wavelet SNR Vs. the RMS delay spread/bit duration Iran 2008
Wavelet-AI Receiver Disadvantages Advantages and
Complexity - many parameters & computations.
High sampling rates - technology limited.
Speed - long simulation times on average machines.
Similar performance to other equalisation techniques.
Data rate independent - data rate changes do not affect structure (just re-train).
Relatively easy to implement with other pulse modulation techniques.
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Visible Light Optical Wireless System with OFDM
Visible-light communication system
Down link Up link Distribution of illuminance Distribution of horizantal illuminance [lx]
Number of LEDs 60 x 60 (4 set)
1400 1200 1000 800 600 400 200 5 4 3 y[m] 2 1 0 0 1 2 x[m] 3 4 5
FSO Network – Two Universities in Newcastle
Agilent Photonic Research Lab
Agilent Photonic Research Lab Research Collaboration A-Block 71 Optical Fibre Free space optical Du-plex communication link (Northumbria and Newcastle Universities) at a data rate of 155 Mbps Iran 2008
Collaborators
• • Graz Technical University, Austria • Houston University, USA • University College London, UK • Hong-Kong Polytechnic University • Tarbiat Modares University, Iran • Newcastle University, UK • Ankara University, Turkey • Agilent, UK • Cable Free, UK • Technological University of Malaysia • Others
Final Remarks
Could the promise of optical wireless live up to reality?
Yes!!
But Optical wireless must complement radio, not compete Industry must be bold in research and development Lower component cost, and single technology based deviced Integration with existing systems Lover receiver sensitivity Of course more
levels research and development at all
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Summary
Access bottleneck has been discussed
FSO introduced as a complementary technology
Atmospheric challenges of FSO highlighted
Subcarrier intensity modulated FSO (with and without spatial diversity) discussed
Wavelet ANN based receivers
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Acknowledgements
To many colleagues (national and international) and in particular to all my MSc and PhD students (past and present) and post-doctoral research fellows
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