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Titlebook: High-Power Lasers and Laser Plasmas / Moshchnye Lazery I Lazernaya Plazma / Мощные Лазеры И Лазерная; N. G. Basov Book 1978 Consultants Bu

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樓主: 小天使
11#
發(fā)表于 2025-3-23 12:33:34 | 只看該作者
Conditions for Obtaining Stationary Lasing with Stimulated Scattering of Lightf these lasers. Until recently, however, it was not clear wheth realized by pulsed pumping. To ascertain the conditions necessary to r we analyzed the operation of the laser under transition conditions [35]. transient can terminate before the end of the pump pulse only if the inte and duration of th
12#
發(fā)表于 2025-3-23 16:42:13 | 只看該作者
13#
發(fā)表于 2025-3-23 22:04:32 | 只看該作者
Single-Frequency SMBS Ring Laseress increases the time required for the steady state to set in and lowers the laser efficiency. On the other hand, the presence of several components greatly hinders the construction of an effectively operating Brillouin laser-amplifier, inasmuch as only the first component is amplified in the ampli
14#
發(fā)表于 2025-3-24 01:46:09 | 只看該作者
15#
發(fā)表于 2025-3-24 06:20:20 | 只看該作者
Q Switching by SMBSors. It is of interest also to consider another situation, where there is a strong coupling between the scattering medium and the source of the exciting light (the laser). In this case the development of the SMBS can cause the laser to go over to the Q-switched regime. We have established that such
16#
發(fā)表于 2025-3-24 08:28:44 | 只看該作者
Inversion of the Exciting-Radiation Wave Front in SMBSerefore be concluded that the light scattered as a result of SMBS propagates backward in the same solid angle as the exciting radiation. This fact was noted earlier [69, 70], but it was never ascertained whether it is due only to the geometry of the experiment or has a more profound nature. To answe
17#
發(fā)表于 2025-3-24 11:35:13 | 只看該作者
18#
發(fā)表于 2025-3-24 16:24:33 | 只看該作者
19#
發(fā)表于 2025-3-24 19:17:43 | 只看該作者
20#
發(fā)表于 2025-3-25 01:50:36 | 只看該作者
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