Proceedings of LFNM ...Institution of Electrical and Electronics Engineers, 2005 - Fiber optics |
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Page 76
... laser radiation is generated as pulses with frequency of following 100 Hz . A radiation pulse shape changes depending on variation of the resonator length within the generation zone . Each pulse of laser radiation can be transformed on ...
... laser radiation is generated as pulses with frequency of following 100 Hz . A radiation pulse shape changes depending on variation of the resonator length within the generation zone . Each pulse of laser radiation can be transformed on ...
Page 78
v is radiation velocity in the resonator , f is radiation frequency , c is light velocity in vacuum , n is absolute ... laser resonator is defined by the expression c c M AL = L1 - L2 = ( v1 − v2 ) M 2 fo n1 n2 2fo - = ( n2 − n1 ) cM ...
v is radiation velocity in the resonator , f is radiation frequency , c is light velocity in vacuum , n is absolute ... laser resonator is defined by the expression c c M AL = L1 - L2 = ( v1 − v2 ) M 2 fo n1 n2 2fo - = ( n2 − n1 ) cM ...
Page 121
... laser radiation and beam heterogeneity at the cross section . Calculation had been carried by approximate formula ( 5 ) ( dashed line at Fig . 2 ) and by searching of extreme value of instantaneous frequency shift with using of ( 2 ) ...
... laser radiation and beam heterogeneity at the cross section . Calculation had been carried by approximate formula ( 5 ) ( dashed line at Fig . 2 ) and by searching of extreme value of instantaneous frequency shift with using of ( 2 ) ...
Contents
LFNM Plenary | 1 |
BatteryLess Spatial Optical Communication Terminals for LocationBased Indoor | 14 |
Resonant Photoproduction of the ElectronPositron Pair with Photon Emission | 27 |
Copyright | |
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