Proceedings of LFNM'...: International Workshop on Laser and Fiber-optical Networks Modeling, Volume 6Institution of Electrical and Electronics Engineers, 2004 - Fiber optics |
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Page 130
... broadening factor ( T ) is expressed as [ 4-5 ] : Γ r = e h 2 ( г 。 + h / t ̧ + h / ) 1+ exp ( ( E , -ħw ) / 2г ) ( 16 ) Where Ex is the transition energy and the half width at half maximum ro , is related to phonon interaction and ...
... broadening factor ( T ) is expressed as [ 4-5 ] : Γ r = e h 2 ( г 。 + h / t ̧ + h / ) 1+ exp ( ( E , -ħw ) / 2г ) ( 16 ) Where Ex is the transition energy and the half width at half maximum ro , is related to phonon interaction and ...
Page 175
... broadening . On the basis of the model considered , it is easy to explain the experimentally observed asymmetry of angular broadening of the anti - Stokes component manifesting itself in the fact that broadening occurs preferentially ...
... broadening . On the basis of the model considered , it is easy to explain the experimentally observed asymmetry of angular broadening of the anti - Stokes component manifesting itself in the fact that broadening occurs preferentially ...
Page 270
... broadening of the beam with a radius of the crossover 1 μm depending on the current is represented on Fig . 1 . 0.0014 0.0012 0,0010 0,0008 0.0006 0.0004 0,0002 0.0000 Ι , ΠΑ 0.0 0,2 0,4 0.6 0.8 1,0 Figure 1 - The plot of the dependence ...
... broadening of the beam with a radius of the crossover 1 μm depending on the current is represented on Fig . 1 . 0.0014 0.0012 0,0010 0,0008 0.0006 0.0004 0,0002 0.0000 Ι , ΠΑ 0.0 0,2 0,4 0.6 0.8 1,0 Figure 1 - The plot of the dependence ...
Contents
L Lasers and Resonators | 1 |
Compact electricdischarge excimer lasers invited | 14 |
Simplified model for XECLlasers | 29 |
Copyright | |
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