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CLIPPING DISTORTION IN LASER DIODE: MODEL, SIMULATIONS AND STATISTICS By: Omar Falou.

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Presentation on theme: "CLIPPING DISTORTION IN LASER DIODE: MODEL, SIMULATIONS AND STATISTICS By: Omar Falou."— Presentation transcript:

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2 CLIPPING DISTORTION IN LASER DIODE: MODEL, SIMULATIONS AND STATISTICS By: Omar Falou

3 Introduction Telecommunications through optical fiber have become a major information- transmission system Networks based on optical fiber technology provides, fast, efficient and reliable means of transmitting information

4 Introduction (cont’d) Optical System: Transmitter, Fiber and Receiver. Transmitter can be either a Light Emitting Diode (LED) or a Laser Diode (LD). LDs have some advantages over LEDs since they are high end, with narrow line width, which make them ideal for long transmission

5 Optical System: an Overview

6 Rayleigh Fading Channel Simulates a wireless communication channel A transmitted signal travels to the receiver along several paths that may have different lengths therefore, different time delays

7 Rayleigh Fading Channel (cont’d) Fading occurs when signals traveling along different paths interfere with each other.

8 Clipping Distortion Clipping distortion has been a subject of interest in many recent studies on frequency-division subcarrier multiplexing (SCM) used in cable television (CATV) applications Clipping occurs when the modulating signal current, which drives the laser diode, occasionally drops below the laser threshold current, turning the laser off (figure on the next slide).

9 Clipping Distortion (cont’d) Region 1: spontaneous emission region Region 2: stimulated emission region or the linear region. Region 3: saturated region.

10 Simulink Model

11 Simulations 2 kinds of fading channel were investigated: –Channel with NO GAIN (0 dB). –Channel with GAIN (effective gain considering all paths is different than 0dB) –Also, for each type of channel, the clipping distortion was studied by varying the number of paths (1, 2, 3, 4 and 5)

12 Fading Channel Simulation Parameters Doppler Frequency: 40 Hz Sample Time: 10 -4 s Path Delay: 0, 10 -3, 2x10 -3, 3x10 -3, 4x10 -3 s Path Gain: 0, -1, -2, -3, -4 Overall Gain: –0 dB –different than 0

13 Results and Analysis

14 Results: Channel with No Gain (1 path) 159/10000 = 1.59 %

15 Results: Channel with No Gain (2 paths) 225/10000 = 2.25 %

16 Results: Channel with No Gain (3 paths) 140/10000 = 1.40 %

17 Results: Channel with No Gain (4 paths) 200/10000 = 2.00 %

18 Results: Channel with No Gain (5 paths) 201/10000 = 2.01 %

19 Results: Channel with Gain (1 path) 201/10000 = 2.01 % 159/10000 = 1.59 %

20 Results: Channel with Gain (2 paths) 201/10000 = 2.01 % 1160/10000 = 11.6 %

21 Results: Channel with Gain (3 paths) 201/10000 = 2.01 % 1842/10000 = 18.42 %

22 Results: Channel with Gain (4 paths) 201/10000 = 2.01 % 2495/10000 = 24.95 %

23 Results: Channel with Gain (5 paths) 201/10000 = 2.01 % 3003/10000 = 30.03 %

24 Results’ Summary

25 Conclusion One of the main problems with using laser diodes is clipping distortion Clipping distortion significantly increases with the increase of number of paths in channel with effective gain However, it remains almost constant for channel with no gains

26 Suggested Solution and Future Work Code the original signal at the transmitter side before modulating in order to minimize or eliminate the effect of clipping Decode the signal at the receiver after it has been demodulated. By doing so, clipped areas of the signal can be detected and recovered.

27 Acknowledgments Dr. Xavier Fernando, Dept. of Electrical and Computer Engineering, Ryerson University Dr. Michael Kolios, Dept. of Math, Physics and Computer Science, Ryerson University


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