氢气退火和离子束抛光后的 1064 纳米波长 (TbBiCa)3Fe5O12 磁光薄膜的性能

Jingyan Yu, Qinghui Yang, Ding Zhang, Xia Xiang, Bo Li, Yong Jiang, Yuanjing Zhang, Han Li, Feng Wang, Shuting Yang, Ihor I. Syvorotka, Huaiwu Zhang
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引用次数: 0

摘要

磁光(MO)材料的激光损伤特性是其应用于近红外(NIR)波段高功率激光系统的最重要限制因素。稀土离子掺杂石榴石(RIG)材料因其优越的磁光特性--小尺寸和低驱动磁场--被广泛应用于光通信系统和紧凑型激光系统。本研究采用液相外延(LPE)方法制备了厚度达数百微米的高质量 (TbBiCa)FeO 薄膜。在还原气氛中退火后,这些薄膜的光吸收比传统的(TbBi)FeO 薄膜更低,同时具有出色的磁光特性,并对其光学和 MO 特性进行了详细研究。然后,对样品进行不同深度的离子束抛光(IBP)处理,并使用原子力显微镜(AFM)观察其表面形貌。最后,采用 R-on-1 方法,用不同频率的多频激光测试了样品的激光诱导损伤阈值(LIDT)。在 50 kHz 的多频激光照射下,(TbBiCa)FeO 的激光诱导损伤阈值为 10.92 J/cm。扫描电子显微镜(SEM)和光学显微镜用于观察损伤后样品的表面形态。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The performace of (TbBiCa)3Fe5O12 magneto-optical films at 1064 nm after hydrogen atmosphere annealing and ion beam polishing
The laser damage properties of magneto-optical (MO) materials are the most important constraint for their application in high-power laser systems in the near-infrared (NIR) band. Rare-earth ion doped garnet (RIG) materials are widely used in optical communication systems and compact laser systems due to their superior MO properties —— small size and low driving magnetic field. In this study, high-quality (TbBiCa)FeO films with hundreds of microns thickness were fabricated by liquid phase epitaxy (LPE) method. These films have lower optical absorption than conventional (TbBi)FeO films after annealing in reducing atmosphere while possessing outstanding magneto-optical properties and their optical and MO properties are investigated in detail, which has a high specific faraday rotation angle of 1413 deg/cm at 1310 nm and 2647 deg/cm at 1064 nm, and transmittance is 51.2 % at 1064 nm and 71.6 % at 1310 nm. After that, ion beam polishing (IBP) treated the samples at different depths, and atomic force microscopy (AFM) was used to observe their surface morphology. Finally, the laser-induced damage threshold (LIDT) of samples was tested by a multi-frequency laser in different frequencies using the R-on-1 method. The LIDT of (TbBiCa)FeO irradiated by a multi-frequency at 50 kHz is 10.92 J/cm. Scanning electron microscopy (SEM) and optical microscopy were used to observe the surface morphology of the sample after the damage.
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