2009
DOI: 10.1134/s0030400x09080244
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On combined diode pumping of a passively Q-switched solid-state laser

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Cited by 2 publications
(3 citation statements)
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“…(6), we should take into account the following circumstances. First, the time τ for an active element in the resonator is shorter than the time τ which is shown in the tables and measured for an active element outside the resonator [15]. Second, the inverted population density n i , which corresponds to the lasing onset time, can be smaller than the activator-ion concentration.…”
Section: Theoretical Modelmentioning
confidence: 80%
“…(6), we should take into account the following circumstances. First, the time τ for an active element in the resonator is shorter than the time τ which is shown in the tables and measured for an active element outside the resonator [15]. Second, the inverted population density n i , which corresponds to the lasing onset time, can be smaller than the activator-ion concentration.…”
Section: Theoretical Modelmentioning
confidence: 80%
“…The high-Q switching corresponding to P a = 0 occurs for the time Δt B = D/V , where D is the effective diameter of the laser-beam cross section in the cell medium, and D ≤ b. The pulse generation of a solid-state laser starts at the instant t 0 when the inverse-population density n(t) [7,10] in the active cell and the threshold density n ia (t) become identical, namely,…”
Section: Actively Q-switched Laser With a Diffraction Cellmentioning
confidence: 99%
“…Then, using the rate equations for a solid-state laser in a way similar to that in [7,10], we obtain the threshold density n ia of inverse population in the active cell…”
Section: Actively Q-switched Laser With a Diffraction Cellmentioning
confidence: 99%