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6 W, 5 mJ amplification with a 28 efficient, kHz, Ti:sapphire regenerative amplifier

机译:6 W,5 MJ扩增,高效,KHz,TI:蓝宝石再生放大器

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The laser design methodology provides the highest energy from a regenerative amplifier possible with a modern pump laser (Quantronix 527 DQ) and minimizes the spectral and phase distortion for a regeneratively amplified ultrafast pulse. In most high-power laser systems, the regenerative amplifier is only a preamplifier that is followed by a multipass amplifier to increase the pulse energy to the several millijoule level. Our regenerative amplifier, however, produces 6 watts of average power at 2 kHz or 5 mJ of pulse energy at 1 kHz. We are aware of no previous Ti:sapphire regenerative amplifier whose average power exceeds 1.5 watts. The regenerative amplifier is a symmetric, two-rod, ring cavity that is stable with pump powers from 0 watts (single shot) to >28 watts. Examine in Fig. 1 the low variance of the cavity mode size at the Ti:sapphire rod and Pockels cell positions as the thermal lens (load) in the gain medium varies. The net input/output energy conversion efficiency for the amplifier is 28±2%. This corresponds to a rod conversion efficiency >34% before losses. Based on our current results and modeling, we believe the laser will produce 8 watts of amplified energy with 28 watts of pump energy. Since the ring cavity amplifies a travelling wave, no amplified pulse energy is sent back to the oscillator. Furthermore, stray reflections in the cavity contribute "postpulse" rather than "prepulse" to the output pulse as required for laser plasma studies. Focusing tests show excellent agreement between a diffraction limited TEM_(00) mode and the amplified spatial mode (see Fig. 2). The high mode quality is ideal for high intensity physics studies.
机译:激光设计方法通过现代泵浦激光(Quantronix 527 DQ)提供来自再生放大器的最高能量,并最大限度地减少再生放大超快脉冲的光谱和相位失真。在大多数高功率激光系统,再生放大器是只后跟一个多程放大器,以增加脉冲能量到几毫焦耳电平的前置放大器。然而,我们的再生放大器在1 kHz的2 kHz或5 MJ的脉冲能中产生6瓦的平均功率。我们知道没有以前的Ti:蓝宝石再生放大器,其平均功率超过1.5瓦。再生放大器是一个对称的双杆,环形腔,其与0瓦(单次)到> 28瓦的泵功率稳定。在图1中检查。在图1中,腔模式尺寸在Ti:蓝宝石杆和袋子电池位置作为增益介质中的热透镜(负载)的低方差变化。放大器的净输入/输出能量转换效率为28±2%。这对应于损耗前的杆转换效率> 34%。基于我们目前的结果和建模,我们认为激光器将产生8瓦的放大能量,具有28瓦的泵能量。由于环腔放大了行波,因此没有放大的脉冲能量被送回振荡器。此外,根据激光等离子体研究的需要,腔体中的杂散反射贡献到输出脉冲的“衰退”而不是“预先完美”。聚焦试验在衍射限量TEM_(00)模式和放大的空间模式之间显示出优异的一致性(参见图2)。高模式质量是高强度物理研究的理想选择。

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