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COMPLEX MODEL OF
    FSO LINKS


      Otakar Wilfert

Brno University of Technology
    Pforzheim, July 2007
Outline

1 Introduction (definition and history)
2 Design of FSO links and their parameters
3 Steady model of the FSO link
4 Statistical model of installation site
5 Complex model
6 Conclusion
Basic characteristics of laser radiation
 high directivity - high concentration of optical power

        TX
                            θ   ≈ 10 −3 rad

Laser
diode

 high monochromatic wave - high concentration of
  information g(ν)
                        Δν          Δν <10 −3
                                    ν
                                  ν

 possibility of quantum state transmission - high degree of
  security during transmission
Definition
  Free-Space optical link (FSO link)
    transmits an optical signal through the
         atmosphere.
    Optical power is concentrated to one
         or more narrow beams
    and optical wave can be divided into
         several optical channels.


(Their application is suitable in situations where the use of
optical cable is impossible and desired bit rate is too high
for a microwave link).
Wave and space division
of optical signal
                                                           transmitting
                                                           lenses
                    Transmitting transceiver
λ1                                    FO             λ1, λ2, …
λ2                λ1, λ2, …                          λ1, λ2, …
         WDM                        Coupler
:                                                    λ1, λ2, …
:                                                    λ1, λ2, …


                  receiving lense
                                       Receiving transceiver

                                                                          λ1
                                               λ1, λ2, …                  λ2
      λ1, λ2, …                                                  WDM
                                                                          :
                                                                          :

                                              4 beams
                                              N-optical channel
                                              2.5 Gb/s in each channel
                                              Fully: N x 2.5 Gb/s
History of optical communication
Bell’s „photophone“ -                 Washington, Franklin Park
The first device in the history which
transmits message by optical beam




    ”FROM THE TOP FLOOR OF THIS BUILDING WAS SENT ON JUNE 3, 1880 OVER A BEAM OF LIGHT TO 1325 L
    STREET THE FIRST WIRELESS TELEPHONE MESSAGE IN THE HISTORY OF THE WORLD. THE APPARATUS
    USED IN SENDING THE MESSAGE WAS THE PHOTOPHONE INVENTED BY ALEXANDER GRAHAM BELL
    INVENTOR OF THE TELEPHONE.“
Bell regarded his photophone as:
   “the greatest invention I have ever made; greater than the telephone”.


                                       source (Sun)
                                                            Principle of Bell’s „photophone“
               modulator
                                                  mirror                       receiver




Bell’s „photophone“ publication:
           Alexander Graham BELL, Ph.D., "On the Production and Reproduction of Sound by Light",
           American Journal of Sciences, Third Series, vol. XX, n°118, Oct. 1880, pp. 305- 324.
A.G. BELL and S. TAINTER, Photophone patent 235,496
granted 1880/12/14




                                Charles                 Alexander
                                Summer Tainter          Graham Bell




                            Authentic drawing of „photophone“ details
However, the radio communications demonstrated by
         Marconi (in 1895) had got bigger progress.


Development of optical communications in free space was made possible
by achievements of semiconductor optoelectronics, fiber optics and laser
technology.
                          Theodor Harold Maiman
                          (invention of laser 1960)




                                                               fotodiodes

Aleksandr Mikhailovich    Nikolai Basov       laser diode
Prokhorov (1916 - 2002)   (1922 - 2001)
       (development of laser diodes - 1962)
1966     Kao and Hockham pointed out that
          long-distance communication
          by fiber is possible




                         Charles K. Kao
                         (born in 1927)

Kao a Fleming in 2004
(Princeton University)



       Today: 0,1dB/km (in spectral window 1550nm)
Bell’s laboratory “today”:

 Scientists and engineers from Bell Labs demonstrated (New Jersey)
 optical link working in free space:

          Range 4,4 km,
          Bit rate 10 Gb/s,
          Wavelength 1550 nm

 Link design includes fiber elements (EDFA, WDM, fiber couplers etc.)



Prototype of multichannels
FSO link (demo picture of progress)




           From history to present day


                       Photophone
Advantages:
the narrow beams guarantee high spatial selectivity so
there is no interference with other links

high bit rate of communication (of 10 Gbit/s)
enables them to be applied in all types of networks

optical band lies outside the area of telecommunication
offices, therefore, a license is not needed for operation

the utilization of quantum state transmission
promises long-term security for high-value data
Disadvantages:
9 availability of FSO link depends on the weather
9 FSO link requires a line of site between transceivers
9 birds and scintillation cause beam interruptions

For reliability improvement number of new methods is
applied:
          1.   Photonic technology
          2.   Multi beam transmission
          3.   Wavelength and space division
          4.   Beam shaping
          5.   Auto-tracking system
          6.   Microwave backup
          7.   Adaptive optics
          8.   Polygonal (mesh) topology
Simplified drawing of the FSO transceiver (example)
FSO link network integration


    Network
    element
              FSO        FSO      Network
                                  element




Transceivers of FSO link are generally protokol transparent


              FSO link substitutes optical fiber
FSO links arrangement
into ”mesh“ topology
Unprofessional activity in area of FSO link

Ronja = Reasonable Optical Near Joint Access




                             “Ronja an User Controlled Technology (like
                             Free Software) project of optical point-
                             to-point data link. The device has 1.4km
                             range and has stable 10Mbps full duplex
                             data rate. Ronja is an optoelectronic
                             device you can mount on your house and
                             connect your PC, home or office network
                             with other networks.“

                             ? BER,
                             ? availability,
                             ? reliability,
http://ronja.twibright.com
                             ? dynamic,
                             ? power margin, …
Some realizations   Laser transmitter
                    (3 beams)




                    Transmitter
                    with LED
                    (1 svazek)




                    Receiver with
                    PIN photodiode
Czech professional activity in the area of FSO links

 ORCAVE - FSO link of the Czech company
 Miracle Group
                                           2 laser beams
                                           auto-tracking system
                                           range 2.0 km @ BER = 10-9
                                           wavelength 1550 nm
                                           management system
                                           monitoring system etc.
ORCAVE - structural design

 2 laser beams              auto-tracking system    installation




 receiver optical system    management system
Commercially obtainable FSO links
Basic characteristics

Examples of commercially obtainable FSO:

Canon (Japan): CANOBEAM DT 50
CBL (Germany): Air Laser
Light Pointe (USA): Flight Spectrum 155/2000
Optical Access (USA): TereScope-OptiLink TS155/DST/CD
SONA Optical Wireless (Canada): SONA beam 155-M
Light Pointe (USA): Flight Strata

            (Parameters of selected FSO follow)
Producer, type                  Canon (Japan)         CBL (Germany)
                                    CANOBEAM               AirLaser
                                       DT 50
                   Bit rate     25 Mb/s to 155 Mb/s         1.25 Gb/s
                                                            125 Mb/s
           Application: a)     Fast Ethernet, ATM etc.   Gigabit Ethernet,
                        b)                                Fast Ethernet
               Range: a)           100 m to 2 km               1 km
                        b)                                     2 km
             Wavelength               785 nm                850 nm

            Class of laser              3B!                  1 M IEC
                                                           (eye safety)
  Optical dynamic range                  ?                    30 dB
              of receiver                                     36 dB
     Interface (fibre): a)            multimode             multimode
                        b)                                 singlemode

                   Backup                 N                     Y


          Remote control                  Y                     Y
    Auto-tracking system                  Y                     N
         Number of beams/                 1/1                  4/1
number of receiving apertura
Producer, type                 LightPointe (USA)      Optical Access (USA)
                                   FlightStrata 155      TereScope-OptiLink
                                                            TS155/DST/CD
                   Bit rate     1.5 Mb/s to 155 Mb/s      10 Mb/s to 155 Mb/s

           Application: a)     Fast Ethernet, ATM etc.    Ethernet, ATM etc.
                        b)
               Range: a)            0 m to 2 km           2.2 km @ 10 dB/km
                        b)                                 1 km @ 30 dB/km
             Wavelength               850 nm                   785 nm

            Class of laser            1 M IEC                   3B!
                                    (eye safety)
  Optical dynamic range                  ?                        ?
              of receiver
      Interface (fibre): a)           singlemode             multimode
                         b)                                  singlemode

                   Backup                 N                       N


          Remote control                  Y                       Y
    Auto-tracking system                  Y                       N
         Number of beams/                 4/4                    3/1
number of receiving aperture
Producer, type                  SONA (Canada)                 Ideal (?)
                                  SONAbeam 155-M          Cost-effective, reliable

                   Bit rate    125 Mb/s to 155 Mb/s       High bit rate (10 Gb/s)
                                                              High secure
           Application: a)     Fast Ethernet, ATM etc.      Transmission of data,
                        b)                               video and high-value data
               Range: a)           200 m to 2 km            Terrestrial: 500 m
                        b)                                  Satellite: 30 000 m
             Wavelength               1550 nm                     WDM

            Class of laser            1 M IEC                   Eye safety
                                    (eye safety)
  Optical dynamic range                36 dB              Availability of 99.99%
              of receiver                                          (?)
     Interface (fibre): a)            multimode                multimode
                        b)                                     singlemode

                   Backup                 N                          Y


          Remote control                  Y                          Y
    Auto-tracking system                  N                        Y(?)
         Number of beams/                 4/1                      4/4(?)
number of receiving aperture                                       +APC
Summary of availability improvement methods
(Pav = 99.9%)
9        (!) the utilization of only photonic elements

9 the utilization of WDM and EDFA

9        (!) multi-beam and multi-aperture transmission

9 “eye safety“ wavelength (1550 nm)

9 greater aperture of transmitting system

9 “auto-tracking“ system (ATS)

9 adaptive power control (APC) for exclusion of saturation

9 optical beam shaping (OBS) for obtaining of top-hat beam

9 the utilization of adaptive optics for reducing of power losses

9 (!) “mesh“ topology and less distance between transceivers

9 (!) microwave backup
Modeling of FSO link
                     Laser beam (without atmosphere)

                     Wave equation is                                    2
                     starting point
                                                                     ∇       E(x, y, z)+ k 2 E(x, y, z) = 0
                                                                                                                        2   2
                                                                                                                       x +y           ⎛             π⎞
                                                                                                   w0        − jk               − j⎜kz+ϕ ( z )−
                     Gaussian beam (laser beam) is
                     one of its solutions                            E(x, y,z) = E0                   e                2q( z )
                                                                                                                               e ⎝           2⎠

                                                                                                  w(z)
                                                                                                                        Utilization of matrix
                                                                                                                        (ABCD law)
                     Gaussian beam is fully characterized                 1 = 1 −j    2
                     by complex parameter                                                                                             Aq1+ B
                                                                         q(z) R(z) kw 2 (z)                                   q 2=
                                                                                                                                      Cq 1+ D
                 Radius curvature of wavefront vs. range                            Beam width vs. range
             5                                                                  6
       4.5

             4                                                                  5

       3.5
                                                                                4
             3

R/z0   2.5                                                               w/w0   3

             2
                                                                                2
       1.5



       0.5
             1
                                                                                1                            θ
             0                                                                  0
                 0    0.5   1   1.5   2   2.5    3   3.5   4   4.5   5              0   0.5   1    1.5   2       2.5      3     3.5       4   4.5   5

                                          z/z0                                                                   z/z0
Optical wave                                             Optical intenzity                                          Optical power
       GG       GG                                   G
                                                                                                              P(z,t) =∫ I(x, y,z,t)dxdy
       E(r,t)×H(r,t)                           =I(r) =I(x, y,z)
                                        time                                                                                   S
       Fast optical changes in time
                                                                                                                   Slow (modulation) changes in time

                                                                 2   2

                                ⎡        ⎤
                                        w0
                                                   2       −2x 2+y                                     Optical intensity distribution
                                                             w (z)
                                                                                                       in Gaussian beam
                                    w(z) ⎥
              I( x, y,z) = I 0 ⎢                       e
                               ⎣               ⎦
        1                                                                                     1

       0.9                                                                                   0.9

       0.8                                                                                   0.8

       0.7                                                                                   0.7

       0.6                                                                                   0.6


I/I0   0.5                                                                            I/I0   0.5

       0.4                                                                                   0.4

       0.3                                                                                   0.3

       0.2                                                                                   0.2

                                                                             e   -2          0.1
       0.1

        0                                                                                     0
         -3        -2    -1         0          1             2           3                         0    0.5    1     1.5   2       2.5   3   3.5   4   4.5   5


                                x/w0                                                                                           z/z0
Laser beam                                  1

                                          0.9

                                          0.8

                                          0.7


Optical intensity distribution            0.6



in Gaussian beam                   I/I0   0.5
                                          0.4

                                          0.3

                                          0.2

                                          0.1                                         e-2
                                            0
                                             -3   -2     -1      0        1   2   3


                                                                x/w




     laser diode


                                 beam




                                                  Speckles in beam spot
Model of power budget
The basic arrangement of the FSO link
                                                               γ tot
         TX            TXA                              RXA
                                 attenuation αtot                             RX
source                                                                             detector
                      P m,TXA              L 12          P m,RXA


                                                                   Psat,RXA
  p(t)        data    (OOK modulation)                    P
                                                                               dynamical
                             Pm,TXA ≈ 1/2 Pimp,TXA                             range Δ
                                                                   P0,RXA
                          t
 All power levels are “mean” value w.r.t. modulation               noise floor
                                           Pm,TXA - mean power radiated through TXA;
  TXA - output aperture                    Pm,RXA - mean power received on RXA;
         of the transmitter;
                                           αtot - total attenuation;
  RXA - input aperture
                                           γtot - total gain;
          of the receiver;                 L12     - distance between TXA and RXA;
Power balance equation and power level diagram
                                               atmosphere
                           beam
          transmitter                                                receiver



                                  Power level diagram
             P
           [dBm]         Pm,TXA α 12
              10                      α~ atm   αatm
                                −γtot
                 0
optical      -10
power                                                               Psat,RXA saturation
                                                                δ   ~
             -20                                                    P m,RXA “clear” atm.
             -30                                                    Pm,RXA      real situation
                                   random                   Δ   M
             -40
                                                                    P0,RXA      sensitivity
                                  Power balance equation

                     Pm,TXA - α12 + γtot - ~atm - αatm = Pm,RXA
Link margin
Graph of link margin
M (L12)                   M(L 12 ) =Pm,PD (L12 ) −P0,PD

                                             Stationary model of
                                             the link by itself




  Link margin is possible to utilize for:
          increasing of range,
          increasing of link immunity against weather
Atmospheric phenomena

Transmission of „clear“
atmosphere

measured at sea level               L12 = 1km; Δλ = 1,5nm




                           Areas
                          applied
Atmospheric phenomena


 Components of αatm

              1. Absorption, scattering and refraction
                   on gas molecules and aerosols (fog, snow, rain)
                   (slow variations)


(λ = 785 nm)        visibility      attenuation      State of the atmosphere
                      [km]           [dB.km-1]
                      < 0.05            > 340              Heavy fog
                    0.2 - 0.5          85 - 34             Middle fog
                    1.0 - 2.0          14 - 7.0      Weak fog or heavy rain
                    2.0 - 4.0          7.0 - 3.0              Haze
                     10 - 23           1.0 - 0.5             Clear
Atmospheric phenomena


Components of αatm

         2. Beam deflection (diurnal variations)
               (temperature or mechanical deformation of consoles)
         3. Short-term interruptions of the beam (short pulses)
               caused by birds, insect,




                                                      1e4



                                                      1e3



                                                      1e2



                                                      10




 (7th floor, filmed from a distance of 750m)           1



                                                       0
                                                       00:00   06:00     12:00      18:00   00:00
                                                                       29/09/2000
Atmospheric phenomena

Components of αatm

            4. Fluctuation of optical intensity (noise-like)
                 caused by air turbulence




    f [Hz]




                                 time of day

            5. Background radiation
FSO testing link

            Bit rate: 155 Mb/s
            Range : 750m
            Single beam

            On-line monitoring:
                            - BER
                            - power levels
                            - meteorological data

            In operation since 1999
Measurements on testing link

                               turbulence, birds, …


Bit error rate (BER)      a)




% Error free sec. (EFS)   b)




                          c)
Received power (Pr)




                                                      fog
Results processing -
statistical model of installation site
                                         100
  PDF of random atmospheric
  attenuation (histogram)                10

  (measured in Autumn)
                                         1




                                         0.1




                                         0
                                              -5   0       5        10          15          20        25        30        35
                                                                          αatm [dB/km]

                                         102

  Exceedance probability function of
  atmospheric attenuation

  This is probability that atmospheric   101

  attenuation exceeds given value



                                         100
                                            0          5       10
                                                                         α
                                                                         15         20
                                                                              atm [dB/km]
                                                                                                 25        30        35
Synthesis of stationary model of the link
and statistical model of installation site




Model of the link:
link margin vs. range



                Availability of the link - complex model
                (model of the given link in selected installation site)
                              100



Model of installation site:
probability that               10




atmospheric attenuation         1                                         λ = 850 nm



exceeds given value
                               0,1




                              0,01
                                     0   20   40   60   80    100   120    140   160   180   200   220   240   260   280   300

                                                             Koeficient útlumu [dB/k m]
Complex model of FSO link

  1                                                          0.01
                 MS=90dB                             Brno

 0.8                                                         0.1
            MS=70dB

 0.6                                                         1


                                               Milesovka
 0.4                                                         10




 0.2                                                          100
       0    20   40   60    80     100   120   140    160   180
                           M1 [dB/km]


Nomogram for unavailability of link assesment
Monitoring of atmospheric phenomena
              in selected sites

Selected                    Czech Republic
sites:
                                         Prague
                                             (750m)
             Brno (950m)
           FSI

                                                      Milesovka hill
                                                      (Donnersberg)

                   FEKT
- Long-term monitoring of
optical power and BER
- Meteorological sensors
Conclusion
9 FSO links are a suitable technology for the ”last mile”
    solution in the frame of access network

9 The utilization of the FSO links is requested namely in
     situations where the use of an optical cable is
     impossible and desired bit rate is too high for a
     microwave links
9 FSO links are flexible, simple and full-value
    (in terms of quality of transmission)
    license-free instrument
    of network communication technologies

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Complex model of fso links

  • 1. COMPLEX MODEL OF FSO LINKS Otakar Wilfert Brno University of Technology Pforzheim, July 2007
  • 2. Outline 1 Introduction (definition and history) 2 Design of FSO links and their parameters 3 Steady model of the FSO link 4 Statistical model of installation site 5 Complex model 6 Conclusion
  • 3. Basic characteristics of laser radiation  high directivity - high concentration of optical power TX θ ≈ 10 −3 rad Laser diode  high monochromatic wave - high concentration of information g(ν) Δν Δν <10 −3 ν ν  possibility of quantum state transmission - high degree of security during transmission
  • 4. Definition Free-Space optical link (FSO link) transmits an optical signal through the atmosphere. Optical power is concentrated to one or more narrow beams and optical wave can be divided into several optical channels. (Their application is suitable in situations where the use of optical cable is impossible and desired bit rate is too high for a microwave link).
  • 5. Wave and space division of optical signal transmitting lenses Transmitting transceiver λ1 FO λ1, λ2, … λ2 λ1, λ2, … λ1, λ2, … WDM Coupler : λ1, λ2, … : λ1, λ2, … receiving lense Receiving transceiver λ1 λ1, λ2, … λ2 λ1, λ2, … WDM : : 4 beams N-optical channel 2.5 Gb/s in each channel Fully: N x 2.5 Gb/s
  • 6. History of optical communication Bell’s „photophone“ - Washington, Franklin Park The first device in the history which transmits message by optical beam ”FROM THE TOP FLOOR OF THIS BUILDING WAS SENT ON JUNE 3, 1880 OVER A BEAM OF LIGHT TO 1325 L STREET THE FIRST WIRELESS TELEPHONE MESSAGE IN THE HISTORY OF THE WORLD. THE APPARATUS USED IN SENDING THE MESSAGE WAS THE PHOTOPHONE INVENTED BY ALEXANDER GRAHAM BELL INVENTOR OF THE TELEPHONE.“
  • 7. Bell regarded his photophone as: “the greatest invention I have ever made; greater than the telephone”. source (Sun) Principle of Bell’s „photophone“ modulator mirror receiver Bell’s „photophone“ publication: Alexander Graham BELL, Ph.D., "On the Production and Reproduction of Sound by Light", American Journal of Sciences, Third Series, vol. XX, n°118, Oct. 1880, pp. 305- 324.
  • 8. A.G. BELL and S. TAINTER, Photophone patent 235,496 granted 1880/12/14 Charles Alexander Summer Tainter Graham Bell Authentic drawing of „photophone“ details
  • 9. However, the radio communications demonstrated by Marconi (in 1895) had got bigger progress. Development of optical communications in free space was made possible by achievements of semiconductor optoelectronics, fiber optics and laser technology. Theodor Harold Maiman (invention of laser 1960) fotodiodes Aleksandr Mikhailovich Nikolai Basov laser diode Prokhorov (1916 - 2002) (1922 - 2001) (development of laser diodes - 1962)
  • 10. 1966 Kao and Hockham pointed out that long-distance communication by fiber is possible Charles K. Kao (born in 1927) Kao a Fleming in 2004 (Princeton University) Today: 0,1dB/km (in spectral window 1550nm)
  • 11. Bell’s laboratory “today”: Scientists and engineers from Bell Labs demonstrated (New Jersey) optical link working in free space: Range 4,4 km, Bit rate 10 Gb/s, Wavelength 1550 nm Link design includes fiber elements (EDFA, WDM, fiber couplers etc.) Prototype of multichannels FSO link (demo picture of progress) From history to present day Photophone
  • 12. Advantages: the narrow beams guarantee high spatial selectivity so there is no interference with other links high bit rate of communication (of 10 Gbit/s) enables them to be applied in all types of networks optical band lies outside the area of telecommunication offices, therefore, a license is not needed for operation the utilization of quantum state transmission promises long-term security for high-value data
  • 13. Disadvantages: 9 availability of FSO link depends on the weather 9 FSO link requires a line of site between transceivers 9 birds and scintillation cause beam interruptions For reliability improvement number of new methods is applied: 1. Photonic technology 2. Multi beam transmission 3. Wavelength and space division 4. Beam shaping 5. Auto-tracking system 6. Microwave backup 7. Adaptive optics 8. Polygonal (mesh) topology
  • 14. Simplified drawing of the FSO transceiver (example)
  • 15. FSO link network integration Network element FSO FSO Network element Transceivers of FSO link are generally protokol transparent FSO link substitutes optical fiber
  • 16. FSO links arrangement into ”mesh“ topology
  • 17. Unprofessional activity in area of FSO link Ronja = Reasonable Optical Near Joint Access “Ronja an User Controlled Technology (like Free Software) project of optical point- to-point data link. The device has 1.4km range and has stable 10Mbps full duplex data rate. Ronja is an optoelectronic device you can mount on your house and connect your PC, home or office network with other networks.“ ? BER, ? availability, ? reliability, http://ronja.twibright.com ? dynamic, ? power margin, …
  • 18. Some realizations Laser transmitter (3 beams) Transmitter with LED (1 svazek) Receiver with PIN photodiode
  • 19. Czech professional activity in the area of FSO links ORCAVE - FSO link of the Czech company Miracle Group  2 laser beams  auto-tracking system  range 2.0 km @ BER = 10-9  wavelength 1550 nm  management system  monitoring system etc.
  • 20. ORCAVE - structural design  2 laser beams  auto-tracking system  installation  receiver optical system  management system
  • 21. Commercially obtainable FSO links Basic characteristics Examples of commercially obtainable FSO: Canon (Japan): CANOBEAM DT 50 CBL (Germany): Air Laser Light Pointe (USA): Flight Spectrum 155/2000 Optical Access (USA): TereScope-OptiLink TS155/DST/CD SONA Optical Wireless (Canada): SONA beam 155-M Light Pointe (USA): Flight Strata (Parameters of selected FSO follow)
  • 22. Producer, type Canon (Japan) CBL (Germany) CANOBEAM AirLaser DT 50 Bit rate 25 Mb/s to 155 Mb/s 1.25 Gb/s 125 Mb/s Application: a) Fast Ethernet, ATM etc. Gigabit Ethernet, b) Fast Ethernet Range: a) 100 m to 2 km 1 km b) 2 km Wavelength 785 nm 850 nm Class of laser 3B! 1 M IEC (eye safety) Optical dynamic range ? 30 dB of receiver 36 dB Interface (fibre): a) multimode multimode b) singlemode Backup N Y Remote control Y Y Auto-tracking system Y N Number of beams/ 1/1 4/1 number of receiving apertura
  • 23. Producer, type LightPointe (USA) Optical Access (USA) FlightStrata 155 TereScope-OptiLink TS155/DST/CD Bit rate 1.5 Mb/s to 155 Mb/s 10 Mb/s to 155 Mb/s Application: a) Fast Ethernet, ATM etc. Ethernet, ATM etc. b) Range: a) 0 m to 2 km 2.2 km @ 10 dB/km b) 1 km @ 30 dB/km Wavelength 850 nm 785 nm Class of laser 1 M IEC 3B! (eye safety) Optical dynamic range ? ? of receiver Interface (fibre): a) singlemode multimode b) singlemode Backup N N Remote control Y Y Auto-tracking system Y N Number of beams/ 4/4 3/1 number of receiving aperture
  • 24. Producer, type SONA (Canada) Ideal (?) SONAbeam 155-M Cost-effective, reliable Bit rate 125 Mb/s to 155 Mb/s High bit rate (10 Gb/s) High secure Application: a) Fast Ethernet, ATM etc. Transmission of data, b) video and high-value data Range: a) 200 m to 2 km Terrestrial: 500 m b) Satellite: 30 000 m Wavelength 1550 nm WDM Class of laser 1 M IEC Eye safety (eye safety) Optical dynamic range 36 dB Availability of 99.99% of receiver (?) Interface (fibre): a) multimode multimode b) singlemode Backup N Y Remote control Y Y Auto-tracking system N Y(?) Number of beams/ 4/1 4/4(?) number of receiving aperture +APC
  • 25. Summary of availability improvement methods (Pav = 99.9%) 9 (!) the utilization of only photonic elements 9 the utilization of WDM and EDFA 9 (!) multi-beam and multi-aperture transmission 9 “eye safety“ wavelength (1550 nm) 9 greater aperture of transmitting system 9 “auto-tracking“ system (ATS) 9 adaptive power control (APC) for exclusion of saturation 9 optical beam shaping (OBS) for obtaining of top-hat beam 9 the utilization of adaptive optics for reducing of power losses 9 (!) “mesh“ topology and less distance between transceivers 9 (!) microwave backup
  • 26. Modeling of FSO link Laser beam (without atmosphere) Wave equation is 2 starting point ∇ E(x, y, z)+ k 2 E(x, y, z) = 0 2 2 x +y ⎛ π⎞ w0 − jk − j⎜kz+ϕ ( z )− Gaussian beam (laser beam) is one of its solutions E(x, y,z) = E0 e 2q( z ) e ⎝ 2⎠ w(z) Utilization of matrix (ABCD law) Gaussian beam is fully characterized 1 = 1 −j 2 by complex parameter Aq1+ B q(z) R(z) kw 2 (z) q 2= Cq 1+ D Radius curvature of wavefront vs. range Beam width vs. range 5 6 4.5 4 5 3.5 4 3 R/z0 2.5 w/w0 3 2 2 1.5 0.5 1 1 θ 0 0 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5 z/z0 z/z0
  • 27. Optical wave Optical intenzity Optical power GG GG G P(z,t) =∫ I(x, y,z,t)dxdy E(r,t)×H(r,t) =I(r) =I(x, y,z) time S Fast optical changes in time Slow (modulation) changes in time 2 2 ⎡ ⎤ w0 2 −2x 2+y Optical intensity distribution w (z) in Gaussian beam w(z) ⎥ I( x, y,z) = I 0 ⎢ e ⎣ ⎦ 1 1 0.9 0.9 0.8 0.8 0.7 0.7 0.6 0.6 I/I0 0.5 I/I0 0.5 0.4 0.4 0.3 0.3 0.2 0.2 e -2 0.1 0.1 0 0 -3 -2 -1 0 1 2 3 0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5 x/w0 z/z0
  • 28. Laser beam 1 0.9 0.8 0.7 Optical intensity distribution 0.6 in Gaussian beam I/I0 0.5 0.4 0.3 0.2 0.1 e-2 0 -3 -2 -1 0 1 2 3 x/w laser diode beam Speckles in beam spot
  • 29. Model of power budget The basic arrangement of the FSO link γ tot TX TXA RXA attenuation αtot RX source detector P m,TXA L 12 P m,RXA Psat,RXA p(t) data (OOK modulation) P dynamical Pm,TXA ≈ 1/2 Pimp,TXA range Δ P0,RXA t All power levels are “mean” value w.r.t. modulation noise floor Pm,TXA - mean power radiated through TXA; TXA - output aperture Pm,RXA - mean power received on RXA; of the transmitter; αtot - total attenuation; RXA - input aperture γtot - total gain; of the receiver; L12 - distance between TXA and RXA;
  • 30. Power balance equation and power level diagram atmosphere beam transmitter receiver Power level diagram P [dBm] Pm,TXA α 12 10 α~ atm αatm −γtot 0 optical -10 power Psat,RXA saturation δ ~ -20 P m,RXA “clear” atm. -30 Pm,RXA real situation random Δ M -40 P0,RXA sensitivity Power balance equation Pm,TXA - α12 + γtot - ~atm - αatm = Pm,RXA
  • 31. Link margin Graph of link margin M (L12) M(L 12 ) =Pm,PD (L12 ) −P0,PD Stationary model of the link by itself Link margin is possible to utilize for: increasing of range, increasing of link immunity against weather
  • 32. Atmospheric phenomena Transmission of „clear“ atmosphere measured at sea level L12 = 1km; Δλ = 1,5nm Areas applied
  • 33. Atmospheric phenomena Components of αatm  1. Absorption, scattering and refraction on gas molecules and aerosols (fog, snow, rain) (slow variations) (λ = 785 nm) visibility attenuation State of the atmosphere [km] [dB.km-1] < 0.05 > 340 Heavy fog 0.2 - 0.5 85 - 34 Middle fog 1.0 - 2.0 14 - 7.0 Weak fog or heavy rain 2.0 - 4.0 7.0 - 3.0 Haze 10 - 23 1.0 - 0.5 Clear
  • 34. Atmospheric phenomena Components of αatm  2. Beam deflection (diurnal variations) (temperature or mechanical deformation of consoles)  3. Short-term interruptions of the beam (short pulses) caused by birds, insect, 1e4 1e3 1e2 10 (7th floor, filmed from a distance of 750m) 1 0 00:00 06:00 12:00 18:00 00:00 29/09/2000
  • 35. Atmospheric phenomena Components of αatm  4. Fluctuation of optical intensity (noise-like) caused by air turbulence f [Hz] time of day  5. Background radiation
  • 36. FSO testing link Bit rate: 155 Mb/s Range : 750m Single beam On-line monitoring: - BER - power levels - meteorological data In operation since 1999
  • 37. Measurements on testing link turbulence, birds, … Bit error rate (BER) a) % Error free sec. (EFS) b) c) Received power (Pr) fog
  • 38. Results processing - statistical model of installation site 100 PDF of random atmospheric attenuation (histogram) 10 (measured in Autumn) 1 0.1 0 -5 0 5 10 15 20 25 30 35 αatm [dB/km] 102 Exceedance probability function of atmospheric attenuation This is probability that atmospheric 101 attenuation exceeds given value 100 0 5 10 α 15 20 atm [dB/km] 25 30 35
  • 39. Synthesis of stationary model of the link and statistical model of installation site Model of the link: link margin vs. range Availability of the link - complex model (model of the given link in selected installation site) 100 Model of installation site: probability that 10 atmospheric attenuation 1 λ = 850 nm exceeds given value 0,1 0,01 0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 Koeficient útlumu [dB/k m]
  • 40. Complex model of FSO link 1 0.01 MS=90dB Brno 0.8 0.1 MS=70dB 0.6 1 Milesovka 0.4 10 0.2 100 0 20 40 60 80 100 120 140 160 180 M1 [dB/km] Nomogram for unavailability of link assesment
  • 41. Monitoring of atmospheric phenomena in selected sites Selected Czech Republic sites: Prague (750m) Brno (950m) FSI Milesovka hill (Donnersberg) FEKT - Long-term monitoring of optical power and BER - Meteorological sensors
  • 42. Conclusion 9 FSO links are a suitable technology for the ”last mile” solution in the frame of access network 9 The utilization of the FSO links is requested namely in situations where the use of an optical cable is impossible and desired bit rate is too high for a microwave links 9 FSO links are flexible, simple and full-value (in terms of quality of transmission) license-free instrument of network communication technologies