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Tunable Cr:Nd:GSGG lasers pumped by red diodes

机译:可调Cr:Nd:GSGG激光器由红色二极管泵浦

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Summary form only given. Laser operation of Nd+3-doped gadolinium scandium gallium garnet (Nd:GSGG) has been first shown by Kaminskii et al. in 1976 [1]. In earlier studies, flaslamp or solar pumping of Nd:GSGG has been explored, and narrow absorption bands of the Nd+3 ion, that overlaps poorly with these broadband emitters resulted in low laser efficiencies. As a solution, co-doping with chromium ion (Cr:Nd:GSGG) has been applied to generate additional broad absorption bands in the visible to improve the absorption as well as the laser efficiency [2-3]. With the development of semiconductor technology, laser diode pumping has become the dominant excitation scheme for Nd-based laser systems [4-6]. Usually, laser diodes at the sharp absorption peaks of Nd:GSSG around 808 nm or 883 nm have been employed [4-5]. As an alternative, Cr co-doped samples provide broad absorption bands around 645 nm, in a spectral region where low cost laser diodes also exist [6]. While using these broad absorption bands, thermal control of the diode junction temperature, narrowband diode operation, and careful selection of diode central wavelength is not required. However, the quantum defect is higher, lowering the laser efficiencies.In this study, we have investigated continuous-wave (cw) and mode-locked laser performance of a red diode pumped Cr:Nd:GSGG laser in detail. State-of-the-art single-mode and multimode laser diodes around 665 nm were used as pump sources. In cw laser experiments, we have demonstrated lasing thresholds as low as 14 mW, slope efficiencies as high as 23.4%, and output powers up to 738 mW (Fig. 1). The free-running laser wavelength was 1061 nm. Using a birefringent tuning plate, lasing could also be obtained at 1051 nm, 1058 nm, 1065 nm, 1068 nm, 1072 nm, 1103 nm and 1111 nm lines. Moreover, two-color and tree-color cw laser operation has been demonstrated in 11 and 3 different transition combinations. In cw mode-locking experiments, a saturable Bragg reflector was used to initiate and sustain pulsing, where the Cr:Nd:GSGG laser produced 6-ps long pulses around 1061 nm, with an average power of 160 mW. The repetition rate was 142.65 MHz, resulting in pulse energies of 1.1 nJ and peak powers of 175 W. Dual-wavelength simultaneous mode-locked operation was also shown for the 1058 nm & 1061 nm lines at an average power of 45 mW. We acknowledge financial support from The Scientific and Technological Research Council of Turkey (114F191).
机译:仅提供摘要表格。 Kaminskii等人首先展示了Nd + 3掺杂g镓镓石榴石(Nd:GSGG)的激光操作。 1976年[1]。在较早的研究中,已经探索了Nd:GSGG的flaslamp或太阳能泵浦技术,Nd + 3离子的窄吸收带与这些宽带发射器重叠很弱,导致激光效率低。作为一种解决方案,已经应用了与铬离子共掺杂(Cr:Nd:GSGG)在可见光中产生附加的宽吸收带,以提高吸收率和激光效率的方法[2-3]。随着半导体技术的发展,激光二极管泵浦已成为基于Nd的激光系统的主要激励方案[4-6]。通常,在808 nm或883 nm附近的Nd:GSSG的吸收峰处使用激光二极管[4-5]。作为替代方案,Cr共掺杂样品在还存在低成本激光二极管的光谱区域中提供645 nm附近的宽吸收带[6]。当使用这些宽吸收带时,不需要对二极管结温度进行热控制,对窄带二极管进行操作以及仔细选择二极管中心波长。然而,量子缺陷较高,降低了激光效率。在这项研究中,我们详细研究了红色二极管泵浦Cr:Nd:GSGG激光器的连续波(cw)和锁模激光性能。约665 nm的最先进的单模和多模激光二极管用作泵浦光源。在连续激光实验中,我们已经证明了激光阈值低至14 mW,斜率效率高达23.4%,输出功率高达738 mW(图1)。自由运行的激光波长为1061 nm。使用双折射调谐板,也可以在1051 nm,1058 nm,1065 nm,1068 nm,1072 nm,1103 nm和1111 nm线处获得激光。此外,已经以11种和3种不同的过渡组合演示了双色和树色连续激光激光器的操作。在连续波锁模实验中,使用了一个可饱和的布拉格反射器来引发和维持脉冲,其中Cr:Nd:GSGG激光器在1061 nm附近产生6 ps长的脉冲,平均功率为160 mW。重复频率为142.65 MHz,产生的脉冲能量为1.1 nJ,峰值功率为175W。在1058 nm和1061 nm的平均功率为45 mW的情况下,还显示了双波长同时锁模操作。我们感谢土耳其科学技术研究委员会(114F191)的财政支持。

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