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Broadband high-efficiency zero-order surface grating coupler for the near- and mid-infrared wavelength ranges

机译:适用于近红外和中红外波长范围的宽带高效零阶表面光栅耦合器

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Efficient coupling of light from a chip into an optical fiber is a major issue in silicon photonics, as the dimensions of high-index-contrast photonic integrated waveguides are much smaller than conventional fiber diameters. Surface grating couplers address the coupling problem by radiating the optical power from a waveguide through the surface of the chip to the optical fiber, or vice versa. However, since the grating radiation angle substantially varies with the wavelength, conventional surface grating couplers cannot offer high coupling efficiency and broad bandwidth simultaneously. To overcome this limitation, for the near-infrared band we have recently proposed SOI-based zero-order grating couplers, which, making use of a subwavelength-engineered waveguide and a high-index prism, suppress the explicit dependence between the radiation angle and the wavelength, achieving a 1-dB bandwidth of 126 nm at λ = 1.55µm. However, in the near-infrared, the bandwidth enhancement of zero-order grating couplers is limited by the effective index wavelength dispersion of the grating. In the mid-infrared spectral region, the waveguide dispersion is lower, alleviating the bandwidth limitation. Here we demonstrate numerically our zero-order grating coupler concept in the mid-infrared at λ = 3.8 urn. Several couplers for the silicon-on-insulator and the germanium-on-silicon nitride platforms are designed and compared, with subdecibel coupling efficiencies and 1-dB bandwidths up to ~680 nm.
机译:从芯片到光的有效耦合到光纤是硅光子学中的一个主要问题,因为高折射率对比光子集成波导的尺寸远小于常规光纤的直径。表面光栅耦合器通过将光功率从波导通过芯片的表面辐射到光纤,反之亦然来解决耦合问题。但是,由于光栅的辐射角基本上随波长变化,所以传统的表面光栅耦合器不能同时提供高耦合效率和宽带宽。为了克服这一限制,对于近红外波段,我们最近提出了基于SOI的零阶光栅耦合器,该耦合器利用亚波长工程波导和高折射率棱镜,抑制了辐射角与入射角之间的显式依赖性。在λ= 1.55µm时达到1dB的带宽126 nm。但是,在近红外中,零阶光栅耦合器的带宽增强受到光栅有效折射率波长色散的限制。在中红外光谱区域中,波导色散较低,从而减轻了带宽限制。在这里,我们在λ= 3.8 urn的中红外数值上演示了零阶光栅耦合器的概念。设计并比较了几种绝缘体上硅和氮化硅上锗平台的耦合器,其耦合效率高达亚分贝,耦合带宽高达1dB,最高可达〜680 nm。

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