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and the polarizer Due to the anisotropic gain of YALO, the beam must be linearly polarized in a speci c direction to obtain the maximum gain Thus a Faraday rotator is used as a part of the optical isolation to preserve linear polarization for the whole double pass Due to the absence of depolarization in the ampli er rods, no second optical isolation for the master oscillator is necessary The system is ashlamp-pumped with a repetition rate of 100 Hz and an excitation time of about 140 ms The master oscillator is based on the system described in Section 44 However, the saturable absorber has a length of 3 mm; thus 13 pulses with a half-width of 90 ns are generated per ash within one burst The ampli ers contain Nd:YALO rods with a dimension of 95 mm 152 mm.
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The total average pump power for both ampli ers is 18 kW Diffuse re ecting pump chambers were used in combination with cerium-doped owtubes to protect the YALO crystals against color center formation The average output power is tunable from 1 W up to 211 W (Fig 435) To increase the average output power, the master oscillator was driven in a TEM00 TEM01 mixed mode The beam diameter is constant within a maximum deviation of 10% for the whole tuning range Figure 436 shows three beam pro les for different average output powers With regard to the advantages of a parallel ampli er setup, a solid-state laser system containing six ampli ers and a master oscillator was developed (Fig 437) The system consists of a parallel arrangement of two double pass ampli cation stages with phase conjugating mirrors.
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