copyright © 2009 arun k. majumdar some challenging areas in free-space laser communications dr....
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Some challenging areas in Free-Space Laser Communications
Dr. Arun K. [email protected]
Lecture Series,: 3
Brno University of Technology, Brno Czech RepublicDecember 1-6, 2009
Review of last lecture: :
• Background, need and recent R&D directions• Basic Free-Space Optics (FSO) communication
system and parameters• Some areas of current interest• My own recent research and results• Conclusions and recommendations for solving
complex problems
Background, need and recent R&D directions Needs for improvements and advanced technologies • laser and hybrid (combination of laser and RF)
communications: advanced techniques and issues • advances in laser beam steering, scanning, and shaping
technologies • laser propagation and tracking in the atmosphere • atmospheric effects on high-data-rate free-space optical data
links (including pulse broadening) • long wavelength free-space laser communications • adaptive optics and other mitigation techniques for free-space
laser communications systems • techniques to mitigate fading and beam breakup due to
atmospheric turbulence/scintillation: spatial, temporal, polarization, and coding diversity strategies, and adaptive approaches
• error correction coding techniques for the atmospheric channel • characterization and modeling of atmospheric effects
(aerosols, turbulence, fog, rain, smoke, etc.) on optical and RF communication links
Background, need and recent R&D directions
(Continued…)• communication using modulated retro-reflection • terminal design aspects for free-space optical link (for
satellite- or land-mobile-terminals) • integration of optical links in networking concepts (e.g.
inter-aircraft MANET) • design and development of flight-worthy and space-
worthy optical communication links • deep-space/ inter-satellite optical communications • multi-input multi-output (MIMO) techniques applied to
FSO • free space optical communications in indoor
environments • underwater and UV communications: applications and
concepts of FSO in sensor networks for monitoring climate change in the air and under water
Basic Free-Space Optics (FSO) communication system and parameters• A typical free-space laser communications
system
Communications Parameters
- Modulation Techniques for FSO communications
- Received signal-to-noise ratio (SNR)
- Bit-Error-Rate
Some areas of current interest
• Atmospheric Turbulence Measurements over Desert site relevant to optical communications systems
• Reconstruction of Unknown Probability Density Function (PDF) of random Intensity Fluctuations from Higher-order Moments
• Atmospheric Propagation Effects relevant to UV Communications
Review of Results and Conclusions• Atmospheric Turbulence Measurements over Desert
site relevant to optical communications systems
H
Air-borne Imaging system
Aberrated wavefront
Spherical wave from point source
Turbulence
Point Source
Strength of Turbulence, Cn2 parameter - Coherence length, r0 - Isoplanatic Angle, Ө0 - Rytov Variance, σr2 - Greenwood Frequency, fG
Atmospheric Models
Hufnagel-Valley (HV) model
Modified Hufnagel-Valley (MHV) model:
•SLC-Day model:
CLEAR1 model:
Temperature fluctuations and Cn2 from
scintillation measurements
1 6 . 6 1 6 . 8 1 7 1 7 . 2 1 7 . 4 1 7 . 6
1 0- 1 5
1 0- 1 4
1 0- 1 3
1 0- 1 2
Cn
2
M i s s i o n D a y / T i m e [ D a y s ]
0.8 1 1.2 1.4 1.6 1.8 2 2.2 2.4 2.61 10
18
1 1017
1 1016
1 1015
1 1014
MeasuredHufnagel-ValleyModified Hufnagel-ValleySLC-DayCLEAR1 Night
Cn2 Profile Comparison
Altitude (Km)
Cn2
(m
^-2/
3)
0.8 1 1.2 1.4 1.6 1.8 2 2.2 2.4 2.61 10
18
1 1017
1 1016
1 1015
1 1014
MeasuredHufnagel-ValleyModified Hufnagel-ValleySLC-DayCLEAR1 Night
Cn2 Profile Comparison
Altitude (Km)
Cn2
(m
^-2/
3)
Comparison of ) Cn2 profile generated from tethered-blimp instrument measurement and various models.
Histogram of Cn2 : some typical examples
14.5 14 13.5 13 12.5 12 11.50
2
4
6
8
log10(Cn2 (m^-2/3))
FR
EQ
UE
NC
Y (
%)
15.5 15 14.5 14 13.5 13 12.50
5
10
log10(Cn2 (m^-2/3))
FR
EQ
UE
NC
Y (
%)
SUMMARY AND CONCLUSIONS
• New results of atmospheric turbulence measurements over desert site using ground-based instruments and tethered-blimp platform are presented
• An accurate model of the complex optical turbulence model for profile is absolutely necessary to analyze and predict the system performance of free-space laser communications and imaging systems
• Because of the complexity and variability of the nature of atmospheric turbulence, accurate measurements of turbulence strength parameters are essential to design the system for operating over a wide range
Review of Results and Conclusions
• Reconstruction of Unknown Probability Density Function (PDF) of random Intensity Fluctuations from Higher-order Moments
PROPOSED METHOD BASED ON HIGHER-ORDER MOMENTS
•sought-for PDF is given by a gamma PDF modulated by a series of generalized Laguerre polynomials:
0 2 4 6 8 10 12 -0.05
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0.45 generalized-Laguerre fit to log-Normal with 6 moments: 10000 data values
ideal PDF PDF fit
PDF(x)
Random Variable, x
0 2 4 6 8 10 12 0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
generalized-Laguerre fit to data LN5000 with 6 moments: 5000 data values
fit nrm histogram
Intensity
CDF
0 2 4 6 8 10 12 -0.05
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
Intensity
generalized-Laguerre fit to data LN5000 with 6 moments: 5000 data values
fit nrm histogram
RESULTS : Simulation using 5000 data samples generated randomly to follow a given distribution
CONCLUSIONS AND SUMMARY
• A new method of reconstructing and predicting an unknown probability density function (PDF) is presented
• The method is based on a series expansion of generalized Laguerre polynomials and generates the PDF from the data moments without any prior knowledge of specific statistics, and converges smoothly
• We have applied this method to both the analytical PDF’s and simulated data, which follow some known non-Gaussian test PDFs such as Log-Normal, Rice-Nakagami and Gamma-Gamma distributions
• Results show excellent agreement of the PDF fit was obtained by the method developed
• The utility of reconstructed PDF relevant to free-space laser communication is pointed out
Review of Results and Conclusions
• Atmospheric Propagation Effects relevant to UV Communications
Monte Carlo Impulse Response Model
Atmospheric Propagation Effects relevant to UV Communications (contd..)
Parametric model (Gamma function) :
3-DB bandwidth:
Related other challenging areas of research and recent developments
• Optical RF Free-Space communications• Underwater optical wireless communications• Indoor optical wireless communications• Chaos-based secure communications• Mitigation of atmospheric turbulence for
communications
Optical RF Free-Space communications
• There is a need for high-capacity communication networks for many applications where it is possible to integrate RF and free space optical hybrid communications
• A robust network• The network is expected to operate under a variety of
weather conditions and through atmospheric distortions
Underwater optical wireless communications
• The present technology of underwater acoustic communication cannot provide high data rate transmission
• Optical wireless communication has been proposed as the best alternative to meet this challenge
• Using the scattered light it is possible to mitigate the communication performance decrease due to absorption only; thus a high data rate underwater optical wireless is a feasible solution
Different communication scenarios
1. Line-of-sight communication link
2. A modulating retro reflector link
3. A reflective link
Underwater optical wireless communication channel properties and link models
• Reference: Shlomi Arnon, “an underwater optical wireless communication Network,” in Free-Space Laser Communications IX edited by Arun K. Majumdar, Christopher Davis, Proc. SPIE Vol. 7464 (2009).
• Extinction coefficient:
Propagation Loss:
Optical signal at the receiver:
1. LOS communication link:
2. Modulating retro-reflector communication link:
Underwater optical wireless communication channel properties and link models (contd..)
3. Reflective communication link:
Approximate received power:
where
Bit Error Rate (BER):
Number of photons and BER as a function of transmitter receiver separation for clean ocean water with extinction
coefficient equal 0.15 m-1
Indoor Optical Communications
• Optical wireless communications as a complementary technology for short-range communications
Website References for Indoor Optical Communications
• Website for “Propagation modeling… Jefffrey Carruthaers ,..):
• http://iss.bu.edu/jbc/Publications/jbc-j7.pdf
• Website for Dominic Obrien “visible light communications: challenges and possibilities”
http://202.194.20.8/proc/PIMRC2008/content/papers/1569135393.pdf
Propagation Modeling for Indoor Optical Wireless Communications
• Impulse response of optical wireless channels• Many receiver or transmitter locations
The transmitter or source Sj, transmitting a signal Xj using intensity modulation, photodiode receiver responsivity r (direct detection), receiver Ri, and Ni(t) is noise at the receiver, he(t;Sj,Ri) is the impulse response of the
channel between source Sj and receiver Ri.
The signal received by receiver Ri is
Source radiant intensity pattern:
Propagation Modeling (contd..)
• Line of sight impulse response:
Where is the distance between the source and the receiver:, and Ari is the optical collection area of the receiver.
Finally, for k bounces, the impulse response for each source Sj is
Where and represent element n acting as a
receiver and a source, and is reflectiviytu of the Lambertiam source
Visible light communications: Indoor linksEmission spectrum of white-light LED Small-signal modulation bandwidth of LED
Transmitter: LED, lens and driver; Channels: LOS and diffuse paths; Receiver: Optics, PD, and amplifiers
Chaos-based Free-space Optical Communications
• Chaotic communication using time-delayed optical systems with EDFRL (erbium-doped fiber ring laser) producing chaotic fluctuations
• Laser with external feedback chaotic optical signal : Optical to opto-electronic feedback
• Mostly fiber optic. Free-space optical communication also (2002 and then 2008)
Fiber-optics based chaos-communications research
Experimental setup for chaotic communication Transmitted and received signals
35 km of single-mode fiber at up to 250 Mbit/s data rate
Reference: Gregory D. Vanwiggeren abd Rajashri Roy, “Chatic communication using time-delayed optical systems,” International Journal of Bifurcation and Chaos< Vol.9, No.11,(1999)
Chaos-based optical communication at high bit rate
Reference: Apostolos Argyris, et al, “Chaos-based communications at high bit rates using commercial fibre-optic link,”Vol.438/17, Nature, November 2005.
Transmission rates in the Gigabit per second range with bit-error rates below 10-7 achieved
Acousto-optic Chaos based secure Free-space Optical Communication Links
Reference: A.K. Ghosh et al, “Design of Acousto-optic Chaos based secure Free-space optical communication links, ”Proc. SPIE Vol.7464, edited by Arun K. Majumdar and Christopher C. Davis, 2009.
Acousto-optic system with electronic feedback:
Shows bistable behavior and can generate chaotic oscillations
Signal Modulation/Encryption with AO Chaos
Basic schemes for optical communications with AO Chaos
-Simpler than laser based chaos encryption systems (external modulator type approach)
- Numerically shown that decryption of the encoded data is possible by using an identical acousto-optic system in the receiver
- Free-space optical communications possible!
Scintillation Mitigation Techniques for Free-Space Optical Communications
• Aperture Averaging
• Spatial Diversity
• Adaptive Optics
• Partially Coherent beams
• Long Wavelength
• Wavelength diversity
• Modulation Schemes
Scintillation Mitigation Techniques (contd..)
• Other Mitigation Techniques– Various Modulation schemes (one example: Polarization Shift
Keying Modulation (POLSK) versus OOK modulation for free-space optical communication) and Forward Error Correction (FEC), Various Coding Schemes
– Partially coherent and Partially polarized beam : for communication
– Long wavelength laser communications (for example: 3.5 μ )