Abstract

An investigation was made of the amplification of microsecond radiation pulses in neodymium-activated glasses. The effective cross sections σeff of stimulated transitions were determined before and after the passage of a high-power pulse. The cross section σeff, representing the active medium at the maximum of a luminescence pulse, was found to depend on the degree of excitation N0 of the active element in the amplifier. When the energy density E0 of the radiation at the amplifier input was increased, the value of σeff (measured after the passage of the pulse being amplified) decreased in the case of silicate glasses, but increased for phosphate glasses. A hypothesis was put forward that the equilibrium profile of the luminescence line of neodymium glasses could become deformed under the action of superluminescence during an optical pump pulse, which would lead to the dependence of σeff on N0. This hypothesis was confirmed by computer calculations carried out on the basis of an approximate model of an active medium with a single inhomogeneously broadened laser transition line and with parameters typical of neodymium glasses. The dependence of the efficiency η of energy extraction on E0 almost reached its maximum value at E0 ≈ 30 J cm-2. A further increase in E0 for the purpose of increasing η would be pointless. The maximum experimental efficiency of extraction of the energy of excited particles was ~95% for phosphate glasses.

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