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Standing-wave saturation resonances

C. Freed and A. Javan, "Standing-Wave Saturation Resonances in the COj 10.6 y Transitions Observed in a Low-Pressure Room-Temperature Absorber Gas," App. Phys. Lett. J 7, 53 (1970). [Pg.159]

Fig.5.24a-d. Spatial intensity distribution for two standing waves with slightly different wavelengths X and A.2 (a), (b), and their corresponding saturation of the inversion AN z) (c). Explanation of spatial hole-burning modes in the active medium (d) with a small length L, close to a resonator mirror Ml (a< b)... [Pg.252]

A laser mode represents a standing wave in the laser resonator with a z-de-pendent field amplitude E(z) as illustrated in Fig.5.20a. Since the saturation of the inversion aN, discussed in the previous section, depends on the inten-sity I JE, the inversion saturated by a single laser mode will exhibit a spatial modulation aN(z) as drawn in Fig.5.20c. Even for a completely homogeneous gain profile, there are always regions of unsaturated inversion... [Pg.256]

Fiq.5.20a-c. Spatial hole burning Field distributions of two standing waves with slightly different wave lengths along the resonator axis and the resultant spatial modulation of the inversion due to gajn saturation... [Pg.257]


See other pages where Standing-wave saturation resonances is mentioned: [Pg.152]    [Pg.152]    [Pg.320]    [Pg.320]    [Pg.211]    [Pg.87]    [Pg.251]    [Pg.291]    [Pg.268]    [Pg.289]    [Pg.44]    [Pg.50]    [Pg.253]    [Pg.64]    [Pg.41]    [Pg.43]    [Pg.75]   


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