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High-performance low-loss fibre polarizer based on graphene and PVB

机译:基于石墨烯和pVB的高性能低损耗光纤偏振器

摘要

Graphene has exceptional electronic transport and photonic properties [1, 2] and as a result this ‘wonder material’ is steadily finding wide-ranging applications in optoelectronic technologies. Although in the short time since its discovery much of the focus has been on its use for electrical devices, more recently a number of graphene-based photonic devices have been demonstrated, including graphene polarizers and electro-absorption based modulators [2, 3]. In this paper, we present a high-performance low-loss broadband fibre polarizer. Previous iterations of such a device require that the optical fibre is polished into the core to provide the required strength of interaction between the graphene sheet and the propagating electromagnetic field, see Fig. 1a [3]. The penalty for this extent of polishing is large device loss (20 dB, at 1550 nm [3]), which has prevented this type of polarizer from becoming a major disruptive technology. With this in mind, we present the first steps towards producing a low-loss in-fibre graphene based polarizer by polishing the fibre close to, but not into, the core. Additional cladding between the fibre core and the graphene sheet reduces the propagation losses but, unfortunately, also decreases the polarizer’s extinction ratio. To address this, we spin coat a polyvinyl butyral (PVB) over-layer onto the graphene which as well as acting as a protective layer, also serves to increase its interaction with the electromagnetic field. A cross-section of the device is shown in Fig. 1b.
机译:石墨烯具有出色的电子传输和光子特性[1,2],因此,这种“奇妙的材料”正在光电技术中稳定地找到广泛的应用。尽管自发现以来在很短的时间内,大部分注意力都集中在其用于电子设备上,但最近已证明了许多基于石墨烯的光子设备,包括石墨烯偏振器和基于电吸收的调制器[2,3]。在本文中,我们提出了一种高性能的低损耗宽带光纤偏振器。这种设备的先前迭代要求将光纤抛光到纤芯中,以提供所需的石墨烯片与传播的电磁场之间的相互作用强度,请参见图1a [3]。这种抛光程度的代价是器件损耗大(在1550 nm处20 dB,[3]),这阻止了这种偏振器成为主要的破坏性技术。考虑到这一点,我们介绍了通过抛光靠近纤芯但不进入纤芯的光纤来生产低损耗的基于石墨烯的偏振器的第一步。纤维纤芯和石墨烯片之间的额外包层减少了传播损耗,但不幸的是,还降低了偏振片的消光比。为了解决这个问题,我们将聚乙烯醇缩丁醛(PVB)覆盖层旋涂到石墨烯上,该石墨烯不仅起着保护层的作用,还增强了其与电磁场的相互作用。该装置的横截面在图1b中示出。

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