Optical amplifier

Download Optical amplifier

Post on 11-May-2015

4.331 views

Category:

Documents

0 download

Embed Size (px)

TRANSCRIPT

<ul><li>1.Optical Amplifiers</li></ul> <p>2. Necessity of Optical amplifiers?To Transmit a signals over long distances (&gt;100km), to compensate attenuation losses.Initially this was accomplished with an optoelectronic module consisting of optical RX, regenerator, equalizer, &amp; an optical TX to send the data.Although functional this arrangement is limited by optical to electrical &amp; electrical to optical conversions. 3. Introduction An optical amplifier is a device whichamplifies the optical signal directlywithout ever changing it to electricity. Thelight itself is amplified. Reasons to use the optical amplifiers: Reliability Flexibility Wavelength Division Multiplexing(WDM) Low Cost 4. Basic ConceptsMost optical amplifiers use stimulated emissionAn optical amplifier is basically a laser without feedbackOptical gain is realized when the amplifier is pumped optically (or electrically) to achieve population inversionGain depends on wavelength, internal light intensity and amplifier mediumThree types: semiconductor optical amplifiers, Raman Amplifiers and fiber doped amplifiers 5. ApplicationsPower AmpConfigurations 6. Selecting AmplifiersMaximumTypeGainNoise figure Output power PowerHigh outputNot veryHigh gainAmplifier power important MediumGood noise In-line Medium gain output powerfigurePreamplifiLow outputLow value &lt; 5Low gainerpowerdB essential 7. Generic optical amplifier Continuous Wave (Constant)Energy is transferred from the pump to signal 8. CoherenceIncoherent light waves Coherent light waves 9. Atomic TransitionsStimulated absorption 10. Stimulated emission 11. Condition for Amplification by Stimulated EmissionPopulation Inversion: More Electrons in higher energy level Pumping: Process to achieve population inversionusually through external energy sourceIn general if N2 &gt; N1 then MEDIA IS SAID TOBE ACTIVE 12. Semiconductor Optical AmplifiersSimilar to Laser diodes but the emission is triggered by input optical signalWork in any wavelength (+)Have high integration, compact and low power consumption (+)Gain fluctuation with signal bit rate (-)Cross talk between different wavelengths (-)Two types: Fabry-Perot or Traveling Wave Amp. 13. Solid State Amplifier Gain VS Power 14. Distributed Fiber AmplifiersThe active medium is created by lightly doping silica fiber core by rare earth element Ex: Erbium (Er)Long fiber length (10-30 m)Low coupling loss (+)Transparent to signal format and bit rateNo cross talkBroad output spectrum (1530 1560 nm) Works only in specific Wavelengths 15. Amplification Process of EDFA N3 N3 Radiationless Decay980 nm N2 N2Pump N1 N1 Optical Pumping to Higher Energy levelsRapid Relaxation to "metastable" State N3~1550 nm~1550 nm N2 Signal N1OutputStimulated Emission and Amplification 16. Fig. 11-4: Erbium energy-level diagram 17. EDFACo-Directional PumpingconfigurationsCounter DirectionalDual Pumping 18. Gain versus EDFA lengthThere is an optimum length that gives the highest gainNegative gain if too long 19. Gain versus pump levelGain decreasesat large signallevelsSignal dependantgainThis increaseswith the pumppower 20. Amplified Spontaneous Emission (ASE) Noise 21. EDFA Noise Figure= (Input SNR)/(Output SNR) 22. SNR degradation due to amplification 23. Fig. 11-12a: Gain-flattened EDFA-A 24. Fig. 11-12b: Gain-flattened EDFA-B 25. Raman Amplifiers Raman Fiber Amplifiers (RFAs) rely on anintrinsic non-linearity in silica fiber Variable wavelength amplification: Depends on pump wavelength For example pumping at 1500 nm producesgain at about 1560-1570 nm RFAs can be used as a standalone amplifier oras a distributed amplifier in conjunction withan EDFA Source: Master 7_5 26. Stimulated Raman ScatteringStimulated Raman Scattering (SRS) causes anew signal (a Stokes wave) to be generatedin the same direction as the pump wavedown-shifted in frequency by 13.2 THz (dueto molecular vibrations) provided that thepump signal is of sufficient strength. 27. Distributed Raman Amplification (I) Raman pumping takes place backwards over the fiber Gain is a maximum close to the receiver and decreases inthe transmitter direction Long Fiber SpanOpticalTransmitter EDFA ReceiverRamanPumpLaser 28. Distributed Raman Amplification (II) With only an EDFA at the transmit end the optical powerlevel decreases over the fiber length With an EDFA and Raman the minimum optical power leveloccurs toward the middle, not the end, of the fiber.EDFA+Raman Optical PowerEDFAonly DistanceSource: Master 7_5 Animation 29. Broadband Amplification using Raman Amplifiers Raman amplification can provides very broadbandamplification Multiple high-power "pump" lasers are used toproduce very high gain over a range of wavelengths. 93 nm bandwidth has been demonstrated with justtwo pumps sources 400 nm bandwidth possible?Source: Master 7_5 30. Advantages and Disadvantages of Raman Amplification Advantages Variable wavelength amplification possible Compatible with installed SM fiber Can be used to "extend" EDFAs Can result in a lower average power over a span, good for lower crosstalk Very broadband operation may be possible Disadvantages High pump power requirements, high pump power lasers have only recently arrived Sophisticated gain control neededSource: Master 7_5 Noise is also an issue 31. ConclusionOptical amplifiers perform a criticalfunction in modern optical networks,enabling the transmission of manyterabits of data over long distances of up tothousands of kilometers. 32. EDFAs 33. SOA 34. Raman Amplifiers 35. Latest technology in Optical Amplifiers 36. References </p>

Recommended

View more >