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Femtosecond laser direct-writing and poling of embedded grating structures

机译:飞秒激光直写和嵌入式光栅结构的极化

摘要

In recent years, the use of a focused femtosecond laser to directly write structures deep within transparent media has attracted much attention due to its ability to write in three-dimensions [1]. By utilizing an amplified Ti:sapphire laser (pulse duration 150fs, repetition rate 250kHz, lambda=850nm), we have developed a novel technique that enables us to write grating structures within the bulk of an optical fiber through its cleaved face, allowing control over light subsequently exiting the fiber. Fig 1(a) shows a microscope image of an embedded diffraction grating having a 5µm pitch and buried 25µm below a fiber's cleaved face. Fig 1(b) displays a far-field pattern created by a single-mode fiber which has a two-dimensional grating written 5µm below its cleaved face. The controllability of the power and direction of diffracting orders offers tantalizing opportunities for new methods of optical routing. A further grating of 20µm period and 4µm line width has been directly-written into a silica glass plate (Herasil 1). Thermal poling was carried out on the plate in air for 15 minutes at 280°C with 4kV applied [2]. After poling the grating was investigated using a Nd:YAG laser (lambda=1064nm), with a focused spot sue of 20µm. The second harmonic was subsequently imaged by CCD camera. Fig 2(a) shows the second harmonic produced in a Gaussian beam away from the grating region as expected. However, Fig 2(b) shows the second harmonic produced at the position of the irradiated lines to be much stronger indicating that the chi(2) is larger in the Ti:Sapphire irradiated regions. The incident beam is large enough to encompass two grating lines as indicated by the arrows. In Fig 2(a) the brightness is enhanced compared to Fig 2(b) to make the spot visible. By direct-writing periodic structures into silica fibers from the side and subsequent poling, work is currently underway to investigate the feasibility of achieving efficient quasi-phase-matching in silica fibres [3]. Fig.1. (a) A 5µm period diffraction grating written 25µm below a fiber's cleaved face. (b) Far-field pattern of single-mode light exiting a fiber containing an embedded 2-d grating. Fig.2. Imaging of the SHG (a) Inclined incidence and well away from the grating. (b) Inclined incidence and on the grating.
机译:近年来,使用聚焦飞秒激光直接在透明介质内部深处写入结构,由于其能够以三维方式进行写入,因此备受关注。[1]通过利用放大的Ti:蓝宝石激光器(脉冲持续时间150fs,重复频率250kHz,λ= 850nm),我们开发了一种新颖的技术,使我们能够通过其劈开面在光纤的主体内写入光栅结构,从而实现对光纤的控制。光线随后从光纤中射出。图1(a)显示了一个嵌入式衍射光栅的显微镜图像,该光栅具有5µm的间距,并埋在光纤劈开面下方的25µm处。图1(b)显示了由单模光纤产生的远场图形,该光纤在其劈开面下方有一个5μm的二维光栅。衍射阶次的功率和方向的可控性为光路由的新方法提供了诱人的机会。另外一个周期为20μm,线宽为4μm的光栅已直接写入石英玻璃板(Herasil 1)。在280°C的空气中,施加4kV电压,在板上进行热极化15分钟[2]。极化后,使用Nd:YAG激光器(λ= 1064nm)对光栅进行了研究,聚焦点为20μm。随后通过CCD相机对二次谐波成像。图2(a)显示了高斯光束在远离光栅区域的情况下所产生的二次谐波。但是,图2(b)显示在辐照线位置产生的二次谐波要强得多,这表明在Ti:蓝宝石辐照区域中chi(2)更大。入射光束足够大,可以包围箭头所示的两条光栅线。在图2(a)中,与图2(b)相比,亮度提高了,从而使斑点可见。通过将周期性结构从侧面直接写入二氧化硅纤维并随后极化,目前正在进行研究以实现在二氧化硅纤维中实现有效的准相位匹配的可行性[3]。图。1。 (a)在光纤劈开面下方25 µm处写入的5 µm周期衍射光栅。 (b)离开包含嵌入式二维光栅的光纤的单模光的远场图案。图2。 SHG的成像(a)倾斜入射且远离光栅。 (b)倾斜入射并在光栅上。

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