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Nd:Gd_(3)Ga_(5)O_(12) waveguide laser fabricated by pulsed laser deposition method with ceramic target

机译:ND:GD_(3)GA_(5)O_(12)波导激光由脉冲激光沉积方法用陶瓷靶制成

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Miniature diode-pumped waveguide laser is promising as a compact and high-efficient coherent light source to convert the poor spatial and spectral mode output of the diode laser into a spatially and spectrally pure low noise beam, that is 'coherence converter'. Since waveguide structure leads to highly efficient laser oscillation by the high optical power densities with a short laser length, diode-pumped waveguide laser will be compact and simple coherent light source. In this paper, we report the fabrication of a crystalline 2 at.% neodymium-doped Gd_(3)Ga_(5)O_(12) (Nd:GGG) film grown upon Y_(3)Al_(5)O_(12) (YAG) substrate by pulsed laser deposition (PLD) method with ceramic target. With crystal target, highly efficient Nd:GGG waveguide laser oscillation has already been reported. PLD is attractive in term of its simple experimental setup and fabrication of waveguide with high numerical aperture (NA). For instance, the GGG (refractive index 1.97) on YAG (1.82) waveguide grown in this work has a NA of 0.75. Such a high-NA waveguide is compatible with coupling to highly divergent laser diode. As a target, we used to Nd_(2)O_(3), Gd_(2)O_(3) and Ga_(2)O_(3) sintered targets. Such a ceramic target is suitable for the control of composition ratio and a good cost performance compared to crystal target. Ceramic sintered target was ablated using KrF eximer laser in the chamber at under 10 mTorr oxygen pressure. KrF eximer laser was used with a repetition rate of 20 Hz and an ablation fluence of 0.5 J/cm~(2). As a substrate, a single crystal YAG cleaned with organic catalyst and etched with sulfuric acid was used and heated at 350°C. Deposited films were post-annealed at 1100°C for four hours. Consequently, as shown in Fig. 1, epitaxial films have been grown.
机译:微型二极管泵浦波导激光器具有紧凑且高效的相干光源,以将二极管激光器的差的空间和光谱模式输出转换为空间和光谱纯低噪声光束,即“相干转换器”。由于波导结构通过具有短的激光长度的高光功率密度来高效的激光振荡,因此二极管泵浦波导激光器将是紧凑且简单的相干光源。在本文中,我们报告了在Y_(3)AL_(5)O_(5)O_(12)上生长的晶体2的制造。%钕掺杂GD_(3)GA_(5)O_(ND:GGG)膜(YAG)基板通过脉冲激光沉积(PLD)方法,具有陶瓷靶标。利用晶体目标,已经报道了高效的Nd:GGG波导激光振荡。 PLD在其简单的实验设置和具有高数值孔径(NA)的波导的简单实验设置和制造中具有吸引力。例如,在该工作中生长的YAG(1.82)波导的GGG(折射率1.97)具有0.75的NA。这种高Na波导与耦合到高度发散的激光二极管兼容。作为目标,我们习惯于ND_(2)O_(3),GD_(2)O_(3)和GA_(2)O_(3)烧结目标。与晶体靶相比,这种陶瓷靶适用于控制组成比和良好的成本性能。在10mTorr氧气压力下使用腔室中的KRF放射线激光烧蚀陶瓷烧结靶。使用20Hz的重复率和0.5J / cm〜(2)的烧蚀剂量进行KRF放大器激光器。作为基材,使用用有机催化剂清洁并用硫酸蚀刻的单晶YAG并在350℃下加热。沉积的薄膜在1100℃下在1100℃下退火4小时。因此,如图1所示。如图1所示,已经生长了外延薄膜。

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