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GeO_2 glass ceramic planar waveguides fabricated by RF-sputtering

机译:射频溅射制备GeO_2玻璃陶瓷平面波导

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摘要

GeO_2 transparent glass ceramic planar waveguides were fabricated by a RF-sputtering technique and then irradiated by a pulsed CO_2 laser. Different techniques like m-line, micro-Raman spectroscopy, atomic force microscopy, and positron annihilation spectroscopy were employed to evaluate the effects of CO_2 laser processing on the optical and structural properties of the waveguides. The GeO_2 planar waveguide after 2h of CO_2 laser irradiation exhibits an increase of 0.04 in the refractive index, measured at 1542 run. Moreover, the technique of laser annealing is demonstrated to significantly reduce propagation loss in GeO_2 planar waveguides due to the reduction of the scattering. Upon irradiation of the surface the roughness decreases from 1.1 to 0.7 nm, as measured by AFM. Attenuation coefficients of 0.7 and 0.5 dB/cm at 1319 and 1542 nm, respectively, were measured after irradiation. Micro-Raman measurements evidence that the system embeds GeO_2 nanocrystals and their phase varies with the irradiation time. Moreover, positron annihilation spectroscopy was used to study the depth profiling of the as prepared and laser annealed samples. The obtained results yielded information on the structural changes produced after the irradiation process inside the waveguiding films of approximately 1 μm thickness.
机译:通过RF溅射技术制备了GeO_2透明玻璃陶瓷平面波导,然后用脉冲CO_2激光辐照。采用了m-线,显微拉曼光谱,原子力显微镜和正电子ni没光谱等不同技术来评估CO_2激光加工对波导光学和结构特性的影响。在1542运行时测得的CO_2激光照射2h后,GeO_2平面波导的折射率增加了0.04。此外,由于散射的减少,激光退火技术被证明可以显着降低GeO_2平面波导中的传播损耗。通过AFM测量,在表面辐射后,粗糙度从1.1nm降低至0.7nm。辐照后,在1319和1542 nm处测得的衰减系数分别为0.7和0.5 dB / cm。显微拉曼测量表明该系统嵌入了GeO_2纳米晶体,并且其相随辐照时间而变化。此外,正电子an没光谱法用于研究所制备和激光退火样品的深度轮廓。所获得的结果产生了关于在大约1μm厚度的波导膜内部进行辐照处理后产生的结构变化的信息。

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  • 来源
    《Optical components and materials XI》|2014年|89820D.1-89820D.12|共12页
  • 会议地点 San Francisco CA(US)
  • 作者单位

    CNR-IFN CSMFO Lab, Via alla Cascata 56/C, Povo, 38123 Trento, Italy;

    IFIMAT, UNCentro and CONICET, Pinto 399, B7000GHG Tandil, Argentina;

    Dipartimento di Fisica, Universita di Trento and INFN, Gruppo collegato di Trento, Via Sommarive 14,I-38123 Povo, Trento, Italy;

    CNR-IFN CSMFO Lab, Via alla Cascata 56/C, Povo, 38123 Trento, Italy,School of Physics, University of Hyderabad, Hyderabad 500046, India,Universita di Trento, Dipartimento di Fisica, via Sommarive 14, Povo, 38123 Trento, Italy;

    CNR-IFN CSMFO Lab, Via alla Cascata 56/C, Povo, 38123 Trento, Italy;

    CNR-IFN CSMFO Lab, Via alla Cascata 56/C, Povo, 38123 Trento, Italy;

    Universita di Trento, Dipartimento di Fisica, via Sommarive 14, Povo, 38123 Trento, Italy;

    Bruno Kessler Foundation and National Research Council Institute of Biophysics, via Sommarive 18, Trento Italy;

    Bruno Kessler Foundation, via Sommarive 18, Trento Italy;

    School of Physics, University of Hyderabad, Hyderabad 500046, India;

    Centro Enrico Fermi;

    IFIMAT, UNCentro and CICPBA, Pinto 399, B7000GHG Tandil, Argentina;

    Dipartimento di Fisica and CNISM, Universita di Trento, Via Sommarive 14, I-38123 Trento, Italy;

    CNR-IFN CSMFO Lab, Via alla Cascata 56/C, Povo, 38123 Trento, Italy;

  • 会议组织
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    Glass ceramic waveguides; CO_2 laser irradiation; Attenuation coefficient; GeO_2 nanocrystals;

    机译:玻璃陶瓷波导; CO_2激光照射;衰减系数GeO_2纳米晶体;

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