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Tunable Cr:Nd:GSGG lasers pumped by red diodes

机译:可调CR:ND:由红色二极管泵送的GSGG激光器

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Summary form only given. Laser operation of Nd<;sup>+3<;/sup>-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<;sup>+3<;/sup> 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:摘要表格仅给出。 Laminskii等人首先显示了Nd <; sup> + 3 <; / sup> -doped gadolinium scandium garnet(nd:gsgg)的激光操作。 1976年[1]。在早期的研究中,已经探索了ND:GSGG的Flaslamp或太阳能泵送,并且Nd <; sup> +3 <; / sup>离子的窄吸收带,与这些宽带发射器重叠,导致激光效率低。作为一种解决方案,已施加与铬离子(Cr:Nd:Gsgg)的共掺杂,以在可见中产生额外的宽吸收带,以改善吸收和激光效率[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的激光系统的主导激励方案[4-6]。通常,在Nd的急剧吸收峰处的激光二极管:GSSG约为808nm或883nm [4-5]。作为替代方案,Cr共掺杂样品在645nm中提供宽的吸收带,在低成本激光二极管的光谱区域中[6]。在使用这些宽吸收带的同时,不需要对二极管结温,窄带二极管操作和仔细选择的二极管中央波长的热控制。然而,量子缺陷较高,降低激光效率。在本研究中,我们已经研究了红色二极管的连续波(CW)和模式锁定的激光性能,详细说明了:Nd:Gsgg激光器。最先进的单模和多模激光二极管左右665 nm用作泵源。在CW激光实验中,我们已经证明了低至14兆瓦,斜坡效率高达23.4 %的激光阈值,输出功率高达738 mW(图1)。自由运行的激光波长为1061nm。使用双折射调节板,也可以在1051nm,1058nm,1065nm,1068nm,1072nm,1103nm和1111nm线中获得激光。此外,在11和3种不同的转换组合中已经证明了两种颜色和树木CW激光操作。在CW模式锁定实验中,使用可饱和布拉格反射器引发和维持脉冲,其中CR:Nd:GSGG激光器产生6-PE长脉冲约为1061nm,平均功率为160mW。重复率为142.65MHz,导致脉冲能量为1.1 NJ,175W的峰值功率为175W。对于1058nm和1061nm线,在45mW的平均功率下也显示了双波长同时锁定操作。我们承认土耳其科技研究委员会(114F191)的财务支持。

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