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EEE 6503 LASER T HEORY C HAPTER -7:: F AST P ULSE P RODUCTION C - PowerPoint PPT Presentation

EEE 6503 LASER T HEORY C HAPTER -7:: F AST P ULSE P RODUCTION C HAPTER -8:: N ONLINEAR O PTICS Presented by, 1 A.F.M. Saniul Haq ID# 0412062205 F AST P ULSE P RODUCTION 2 I NTRODUCTION LASERs are widely used for marking, cutting, drilling.


  1. EEE 6503 LASER T HEORY C HAPTER -7:: F AST P ULSE P RODUCTION C HAPTER -8:: N ONLINEAR O PTICS Presented by, 1 A.F.M. Saniul Haq ID# 0412062205

  2. F AST P ULSE P RODUCTION 2

  3. I NTRODUCTION � LASERs are widely used for marking, cutting, drilling. � Works on the principle of vaporizing material � CW LASER tends to heat the surrounding area of target and also can damage substrate. target and also can damage substrate. � Short pulses are best for controlled operation. � Fast, powerful pulses tend to ablate material quickly without heating. � For many operation, the shorter the pulse the better. FAST PULSE PRODUCTION 3

  4. F AST -P ULSE P RODUCTION � Simplest technique envisioned is to switch the gain of the medium on and off. � Its done by switching pump energy on and off. � The problem with the scheme: � Delay for population inversion � Delay for population inversion � Sets limit in the pulse length and repetition time Q-Switching Technique 4

  5. C ONCEPT OF Q-S WITCHING � LASER output is controlled by switching loss in the medium � Also called Loss Switching . � Loss is inserted in the cavity and hence output is spoiled. spoiled. � Q-switch can be thought of as an optical gate blocking optical path 5

  6. I NTRACAVITY S WITCHES • synchronization Rotating Mirror • Linear Q-value • controlled EO or AO switch • Sharp Q-change • organic Saturable dye switch Saturable dye switch • Q varies with lifetime • Q varies with lifetime 6

  7. E NERGY S TORAGE � 7

  8. P OPULATION I NVERSION � 8

  9. P ULSE P OWER AND E NERGY � Lifetime of the photon in cavity Lifetime of the photon in cavity 9

  10. P ULSE P OWER AND E NERGY � 10

  11. P ULSE P OWER AND E NERGY � Integrating constant 11

  12. P ULSE P OWER AND E NERGY � 12

  13. P ULSE P OWER AND E NERGY � 13

  14. P ULSE P OWER AND E NERGY � 14

  15. P ULSE P OWER AND E NERGY � 15

  16. E LECTROOPTIC M ODULATOR � EO modulators works on the principle of birefringence. � Separates incident light ray into two rays that may travel in different direction. � It is also called Double Refraction . � Calcite is natural crystal that exhibits birefringence. Calcite is natural crystal that exhibits birefringence. 16

  17. E LECTROOPTIC M ODULATOR � 17

  18. E LECTROOPTIC E FFECT � Linear EO coefficient Second order EO coefficient 18

  19. E LECTROOPTIC M ODULATOR 19

  20. E LECTROOPTIC M ODULATOR � 20

  21. EO M ODULATOR � Fastest Q-switch :: feature switching time 10ns. � Large hold-of or extinction ratio :: as high as 1000:1 � Suitable EO crystals :: very expensive Driver circuitry :: very critical � High voltage capacitors required 21

  22. A COUSTOOPTIC M ODULATOR � Simplest modulator � Acoustic wave originated from piezoelectric crystal 22

  23. A COUSTOOPTIC M ODULATOR 23

  24. D IFFRACTION � 24

  25. R AMAN -N ATH D IFFRACTION � Incoming beams are perpendicular to alternating layers. � Act like parallel slits of transmission diffraction grating. 25

  26. AO M ODULATOR � Requires RF drive signal at 27 to 28 MHz and minimum power of 10 W � Low hold-of ratio :: about 10% loss in the central beam. 26

  27. C AVITY D UMPING 27

  28. M ODELOCKING 28

  29. M ODELOCKING IN F REQUENCY D OMAIN 29

  30. M ODELOCKING IN F REQUENCY D OMAIN 30

  31. N ON -L INEAR O PTICS 31

  32. L INEAR AND N ONLINEAR P HENOMENA 32

  33. P OLARIZATION � Non-linear coefficient Linear coefficient 33

  34. P OLARIZATION 34

  35. P OLARIZATION 35

  36. SHG 36

  37. P HASE M ATCHING 37

  38. P HASE M ATCHING � 38

  39. N ON - LINEAR I NTERACTION � Mixing of two lights beam � sum or difference freq. � Phase matching is required in crystal for this. � Non-linear crystals are of 2 types: � Type-I � Type-II 39

  40. T YPE OF C RYSTAL 40

  41. E X . O F P HASE M ATCHING WHY? 41

  42. N ON - LINEAR M ATERIAL � 42

  43. N ON - LINEAR M ATERIAL � 43

  44. SHG E FFICIENCY � Length of crystal Area of the beam 44

  45. O PTICAL M IXING 45

  46. H IGHER -O RDER N ONLINEAR E FFECT 46

  47. O PTICAL P ARAMETRIC O SCILAATION 47

  48. 48

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