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Lecture 6. Polarization splitter based Filters Acoustooptic Tunable Filters.

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Presentation on theme: "Lecture 6. Polarization splitter based Filters Acoustooptic Tunable Filters."— Presentation transcript:

1 Lecture 6

2 Polarization splitter based Filters

3 Acoustooptic Tunable Filters

4 Electrooptic Tunable Filters

5 Tunable Add-Drop Filters Phase matched AOTF : changing f for tuning EOTF: changing V for tuning.

6 Laser Diodes

7 Direct modulation: easy to implement but causing spectral broadening which can reduce bandwidth for long distance transmission. External modulation: Overcoming excess spectral broadening, at cost of increased transmitter cost of complexity.

8 Laser Diodes Two key features of laser operation Gain: stimulated emission of light. Oscillation: resonant cavity.

9 Fabry-Perot model of laser

10 After one round trip After N round trips

11 Fabry-Perot model of laser N   : steady state

12 Fabry-Perot model of laser

13

14 Relate Δ  to spectral characteristic

15 Fabry-Perot model of laser Recall N = group refractive index

16 Fabry-Perot model of laser

17

18 How does total output power in a mode depend on  ?

19 Fabry-Perot model of laser Output power in mode varies as 1/ .

20 Fabry-Perot model of laser

21 Example 1 What is the longitudinal mode spacing in Angstroms and Hz, for an InGaAsP Fabry-Perot laser emitting at a wavelength of 1.53 μ m, with N = 4 and L = 300 μ m?

22 Example 2 From previous example, what is the total spectral width of the laser emission, in Angstroms and Hz, if the laser emission contains seven longitudinal modes?

23 Laser Rate Equations N = number of carriers (e-h pairs) in active region. S = number of photons in cavity in lasing mode. J = current for pumping diode. e = electronic charge = 1.6 x 10 -19 C.  sp = spontaneous lifetime of carriers. N 0 = number of carriers for transparency  = fraction of spontaneous emission coupled into lasing mode.  ph = photon lifetime in cavity. g = gain coefficient.

24 Laser Rate Equations Steady state: For small current (S  0)

25 Laser Rate Equations Lasing threshold:

26 Laser Rate Equations Above threshold:

27 Laser Rate Equations

28 Example 3 Parameters for a semiconductor laser are: What is the photon lifetime? What is the number of carriers at lasing threshold?

29 Laser Rate Equations How long does a photon stay in cavity?

30 Laser Rate Equations

31 Example 4 What is the power gain coefficient in cm -1 in a semiconductor FP laser operating above threshold with a cavity length of 250 μ m and facet reflectances of R 1 =R 2 = 1%. In both cases assume that the gain is a constant within the cavity.


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