Fabrication of sub-micron Thick, low loss As2S3 planar waveguides

D. Choi, S. Madden, D. Bulla, Rongping Wang, A. Rode, B. Luther-Davies
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Abstract

A chalcogenide glass (ChG) is one containing the chalcogen elements (Sulphur, Selenium or Tellerium) as a substantial constituent covalently bonded to network forming elements such as Germanium, Arsenic, or Antimony. ChG films are emerging as good candidates for integrated nonlinear optic (NLO) devices due to their high optical nonlinearities and low linear and nonlinear losses. We had already developed 2−3 micron thick As2S3 waveguides employing semiconductor processing [1] and demonstrated several NLO devices [2]. For more compact photonic integrated circuits, however, the device length reduction has to be compensated by boosting the waveguide nonlinearity coefficient, γ = (2π/λ)(n2/Aeff). The nonlinear refractive index, n2, is inherent to a material; hence the effective area of the light in the guide (Aeff) should be shrunk. This means the propagating light is to be confined tightly in the structure. The aim of this study, therefore, was to fabricate sub-micron thick, compact waveguides having low propagation loss.
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亚微米厚、低损耗As2S3平面波导的制备
硫系玻璃(ChG)是一种含有硫元素(硫、硒或碲)的玻璃,其实质成分与锗、砷或锑等网状元素共价结合。ChG薄膜由于其高光学非线性和低线性和非线性损耗而成为集成非线性光学(NLO)器件的良好候选者。我们已经采用半导体工艺开发了2 - 3微米厚的As2S3波导[1],并演示了几种NLO器件[2]。然而,对于更紧凑的光子集成电路,器件长度的减少必须通过提高波导非线性系数γ = (2π/λ)(n2/Aeff)来补偿。非线性折射率n2是材料固有的;因此,导光片的有效面积(Aeff)应该缩小。这意味着传播的光将被紧紧地限制在结构中。因此,本研究的目的是制造亚微米厚、紧凑、传播损耗低的波导。
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