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[object Object]
Stimulated emission Spontaneous emission L ight  A mplification by  S timulated  E mission of  R adiation
Energy level diagram ,[object Object]
[object Object],[object Object],[object Object],[object Object],T he operation of the Laser
T he operation of the Laser
T he operation of the Laser (Pumping the Laser)
T he operation of the Laser absorption
T he operation of the Laser Spontaneous emission
T he operation of the Laser Spontaneous emission ,[object Object],[object Object]
T he operation of the Laser
T he operation of the Laser Stimulated emission
T he operation of the Laser Light: Coherent, polarized The stimulating and emitted photons have the same: frequency phase direction
Two level system absorption Spontaneous emission Stimulated emission h  h  h  E 1 E 2 E 1 E 2 h  =E 2 -E 1
[object Object],[object Object],Boltzmann’s equation example:  T=3000 K  E 2 -E 1 = 2.0 eV E 1 E 2
Einstein’s coefficients   Probability of stimulated absorption R 1-2   R 1-2  =    (  ) B 1-2    Probability of stimulated  and spontaneous emission  : R 2-1  =    (  ) B 2-1  + A 2-1     assumption: n 1   atoms of energy   1  and  n 2  atoms of energy   2  are in thermal equilibrium at temperature T with the  radiation of spectral density    (  ):   n 1  R 1-2  =  n 2  R 2-1   n 1   (  ) B 1-2  = n 2  (   (  ) B 2-1  + A 2-1 )     E 1 E 2
B 1-2 /B 2-1  = 1   ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],            Planck’s law
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],  x ~  n 2 /n 1      
Condition for the laser operation If   n 1  >  n 2 ,[object Object],[object Object],[object Object],[object Object],[object Object],if  n 2   > >  n 1   -  population  inversion Necessary condition:   population inversion E 1 E 2
How to realize the population inversion? Thermal excitation:  Optically,   electrically . impossible. The system has to be „pumped” E 1 E 2
Measurement disturbes the system The Uncertainty Principle
The Uncertainty Principle ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
The Uncertainty Principle ,[object Object]
Three level laser The laser operation E 1 E 3 E 2 Fast transition Laser action ,[object Object],[object Object],[object Object],[object Object],[object Object]
E 1 E 3 E 2 szybkie przejścia akcja laserowa - optical pumping - occupation of E3  of a short life time,  10-8s. It is a band, the metastable and ground states are narrow : -  electrons are collected on E2: population inversion  -   stimulated emission (one photon emitted spontaneously starts the stimulated radiation ) - Beam of photons moves normally to the mirrors – standing wave.  The laser operation
 
ruby laser ,[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],rapid decay Ruby laser Al 2 O 3 Cr + Energy 4 A 2 4 T 2 4 T 1 2 T 2 2 E LASING
Ruby laser First laser:  Ted Maiman Hughes Research Labs 1960

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Presentation of the OECD Artificial Intelligence Review of GermanyPresentation of the OECD Artificial Intelligence Review of Germany
Presentation of the OECD Artificial Intelligence Review of Germany
 

Laser

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  • 2. Stimulated emission Spontaneous emission L ight A mplification by S timulated E mission of R adiation
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  • 5. T he operation of the Laser
  • 6. T he operation of the Laser (Pumping the Laser)
  • 7. T he operation of the Laser absorption
  • 8. T he operation of the Laser Spontaneous emission
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  • 10. T he operation of the Laser
  • 11. T he operation of the Laser Stimulated emission
  • 12. T he operation of the Laser Light: Coherent, polarized The stimulating and emitted photons have the same: frequency phase direction
  • 13. Two level system absorption Spontaneous emission Stimulated emission h  h  h  E 1 E 2 E 1 E 2 h  =E 2 -E 1
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  • 15. Einstein’s coefficients   Probability of stimulated absorption R 1-2 R 1-2 =  (  ) B 1-2   Probability of stimulated and spontaneous emission : R 2-1 =  (  ) B 2-1 + A 2-1   assumption: n 1 atoms of energy  1 and n 2 atoms of energy  2 are in thermal equilibrium at temperature T with the radiation of spectral density  (  ):   n 1 R 1-2 = n 2 R 2-1 n 1  (  ) B 1-2 = n 2 (  (  ) B 2-1 + A 2-1 )     E 1 E 2
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  • 19. How to realize the population inversion? Thermal excitation: Optically, electrically . impossible. The system has to be „pumped” E 1 E 2
  • 20. Measurement disturbes the system The Uncertainty Principle
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  • 24. E 1 E 3 E 2 szybkie przejścia akcja laserowa - optical pumping - occupation of E3 of a short life time, 10-8s. It is a band, the metastable and ground states are narrow : -  electrons are collected on E2: population inversion -   stimulated emission (one photon emitted spontaneously starts the stimulated radiation ) - Beam of photons moves normally to the mirrors – standing wave. The laser operation
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  • 28. Ruby laser First laser: Ted Maiman Hughes Research Labs 1960