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CN105759348A - Silica-based double-section type groove waveguide polarization rotator and polarization rotation method - Google Patents

Silica-based double-section type groove waveguide polarization rotator and polarization rotation method Download PDF

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CN105759348A
CN105759348A CN201610327983.9A CN201610327983A CN105759348A CN 105759348 A CN105759348 A CN 105759348A CN 201610327983 A CN201610327983 A CN 201610327983A CN 105759348 A CN105759348 A CN 105759348A
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waveguide
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slot waveguide
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CN105759348B (en
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肖金标
徐银
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Southeast University
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/105Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type having optical polarisation effects
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/26Optical coupling means
    • G02B6/27Optical coupling means with polarisation selective and adjusting means
    • G02B6/2753Optical coupling means with polarisation selective and adjusting means characterised by their function or use, i.e. of the complete device
    • G02B6/2766Manipulating the plane of polarisation from one input polarisation to another output polarisation, e.g. polarisation rotators, linear to circular polarisation converters

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  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Integrated Circuits (AREA)

Abstract

本发明提出一种硅基双段式槽波导偏振旋转器和偏振旋转方法,包括槽波导和尺寸相同的第一至第四条形波导;第一、第二条形波导为一组形成第一偏振旋转区,第三、第四条形波导为一组形成第二偏振旋转区,第一、第二偏振旋转区顺次连接;成为一组的两条形波导分置槽波导两侧,且第一、第三条形波导位于槽波导的同一侧,第二、第四条形波导位于槽波导的另一侧;第一、第四条形波导顶面与槽波导顶面平齐,第二、第三条形波导底面与槽波导底面相平齐。对于包含任意偏振态的输入光信号在经过该器件的第一和第二偏振旋转区之后,在输出端能够输出与之正交的另一偏振态光信号,从而实现偏振旋转的功能。

The present invention proposes a silicon-based two-stage slot waveguide polarization rotator and polarization rotation method, including a slot waveguide and first to fourth strip waveguides with the same size; the first and second strip waveguides form a first In the polarization rotation area, the third and fourth strip waveguides form a second polarization rotation area as a group, and the first and second polarization rotation areas are connected in sequence; two waveguides forming a group are placed on both sides of the slot waveguide, and The first and third strip waveguides are located on the same side of the slot waveguide, and the second and fourth strip waveguides are located on the other side of the slot waveguide; the top surfaces of the first and fourth strip waveguides are flush with the top surface of the slot waveguide; 2. The bottom surface of the third strip waveguide is flush with the bottom surface of the slot waveguide. For an input optical signal containing any polarization state, after passing through the first and second polarization rotation regions of the device, another polarization state optical signal orthogonal to it can be output at the output end, thereby realizing the function of polarization rotation.

Description

一种硅基双段式槽波导偏振旋转器和偏振旋转方法A silicon-based two-stage slot waveguide polarization rotator and polarization rotation method

技术领域technical field

本发明涉及集成光学技术领域,具体涉及一种硅基双段式槽波导偏振旋转器和偏振旋转方法。The invention relates to the technical field of integrated optics, in particular to a silicon-based double-section slot waveguide polarization rotator and a polarization rotation method.

背景技术Background technique

光子集成回路技术近年来飞速发展,特别是基于绝缘体上硅(Silicon-on-insulator,SOI)材料平台,在构建片上超紧凑、高性能、低功耗、低成本的光集成器件和系统方面受到了研究人员的广泛关注。但是SOI材料固有的高折射率差特性不可避免地会给器件和系统的设计带来明显的结构双折射效应,产生强烈的偏振相关性,这将极大地限制光子集成回路在片上光通信中的大规模商业化应用。为此,片上偏振分集方案被提出用以实现偏振透明传输,而偏振分束器和旋转器是其中的必备部件。针对偏振旋转器,目前研究人员已经提出了众多的器件方案,包括采用非对称定向耦合器、非对称倾斜波导、亚波长狭缝、光子晶体结构和电光/磁光材料等,用以改变结构或者材料的垂直对称性,进而实现偏振态旋转的功能。现阶段偏振旋转器还存在一些问题,特别是尺寸较大、偏振旋转效率较低和对工艺制作要求较高等,所以需要找寻新的方法以有效提高器件的整体性能,为实现片上高密度偏振无关传输及高速偏振复用传输奠定基础。Photonic integrated circuit technology has developed rapidly in recent years, especially based on the silicon-on-insulator (SOI) material platform, which has received great attention in the construction of on-chip ultra-compact, high-performance, low-power, and low-cost optical integrated devices and systems. received extensive attention from researchers. However, the inherent high refractive index difference of SOI materials will inevitably bring obvious structural birefringence effects to the design of devices and systems, resulting in strong polarization dependence, which will greatly limit the application of photonic integrated circuits in on-chip optical communication. Large-scale commercial application. To this end, an on-chip polarization diversity scheme is proposed to achieve polarization transparent transmission, and polarization beam splitters and rotators are essential components. For polarization rotators, researchers have proposed many device solutions, including asymmetric directional couplers, asymmetric inclined waveguides, sub-wavelength slits, photonic crystal structures, and electro-optical/magneto-optical materials, etc., to change the structure or The vertical symmetry of the material realizes the function of polarization state rotation. At this stage, there are still some problems in the polarization rotator, especially the large size, low polarization rotation efficiency and high requirements on the process. Therefore, it is necessary to find new methods to effectively improve the overall performance of the device. In order to achieve high-density polarization independent on-chip transmission and high-speed polarization multiplexing transmission to lay the foundation.

最近,一种新颖的波导结构—槽波导被提出,基于其特殊的结构,能够获得显著的场增强效应和局域场分布特性。如今,这种波导已经被用于多种有源和无源器件中,包括:有机混合光调制器、定向耦合器、微环谐振器、多模干涉耦合器、分束器和传感器等。在这些器件中,主要利用了槽波导的场增强效应模式,以有效提高器件的灵敏度、耦合效率、工作带宽等。考虑到槽波导也是偏振敏感性结构,其偏振相关性甚至比普通的硅基纳米线更强,所以在利用槽波导构建片上光子集成回路时,偏振管理是一个急需解决的关键问题,在实际运用中,我们需要将槽波导的另一个偏振模式转为具有场增强效应的模式,从而使得其在功能器件中的优势更加明显。据此,针对槽波导,设计一种具有尺寸小、工作带宽大、偏振旋转效率高、插入损耗低的偏振旋转器显得十分重要。Recently, a novel waveguide structure—slot waveguide was proposed. Based on its special structure, it can obtain significant field enhancement effect and local field distribution characteristics. Today, such waveguides have been used in a variety of active and passive devices, including: organic hybrid optical modulators, directional couplers, microring resonators, multimode interference couplers, beam splitters, and sensors. In these devices, the field enhancement effect mode of the slot waveguide is mainly used to effectively improve the sensitivity, coupling efficiency, and working bandwidth of the device. Considering that the slot waveguide is also a polarization-sensitive structure, its polarization dependence is even stronger than that of ordinary silicon-based nanowires. Therefore, when using slot waveguides to construct on-chip photonic integrated circuits, polarization management is a key issue that needs to be solved urgently. In practical applications In , we need to convert the other polarization mode of the slot waveguide into a mode with field enhancement effect, so that its advantages in functional devices are more obvious. Accordingly, for the slot waveguide, it is very important to design a polarization rotator with small size, large working bandwidth, high polarization rotation efficiency and low insertion loss.

发明内容Contents of the invention

发明目的:为解决上述技术问题,提供一种尺寸小、工作带宽大、偏振旋转效率高、插入损耗低的偏振旋转器,本发明提出一种硅基双段式槽波导偏振旋转器和偏振旋转方法。Purpose of the invention: In order to solve the above technical problems, provide a polarization rotator with small size, large working bandwidth, high polarization rotation efficiency and low insertion loss. This invention proposes a silicon-based double-stage slot waveguide polarization rotator and method.

技术方案:为实现上述技术效果,本发明提出的技术方案为:Technical scheme: in order to realize above-mentioned technical effect, the technical scheme that the present invention proposes is:

一种硅基双段式槽波导偏振旋转器,它包括槽波导和尺寸相同的第一条形波导4、第二条形波导5、第三条形波导6、和第四条形波导7;所述槽波导延长度方向分为输入槽波导1、传输槽波导2和输出槽波导3;传输槽波导2沿长度方向均分为两段:第一传输段和第二传输段,其中,第一传输段两侧分别设有位置相对的第一条形波导4和第二条形波导5,第一条形波导4的顶面与传输槽波导2顶面相平齐,第二条形波导5的底面与传输槽波导2底面相平齐;第二传输段两侧分别设有位置相对的第三条形波导6和第四条形波导7,第三条形波导6的底面与传输槽波导2底面相平齐,第四条形波导7的顶面与传输槽波导2顶面相平齐;第一条形波导4和第三条形波导6位于传输槽波导2的同一侧,第二条形波导5和第四条形波导7位于传输槽波导2的另一侧。A silicon-based double-section slot waveguide polarization rotator, which includes a slot waveguide and a first strip waveguide 4, a second strip waveguide 5, a third strip waveguide 6, and a fourth strip waveguide 7 of the same size; The elongation direction of the slot waveguide is divided into an input slot waveguide 1, a transmission slot waveguide 2 and an output slot waveguide 3; the transmission slot waveguide 2 is equally divided into two sections along the length direction: the first transmission section and the second transmission section, wherein, the first transmission section and the second transmission section A first strip waveguide 4 and a second strip waveguide 5 opposite to each other are respectively arranged on both sides of a transmission section, the top surface of the first strip waveguide 4 is flush with the top surface of the transmission groove waveguide 2, and the second strip waveguide 5 The bottom surface of the second transmission section is flush with the bottom surface of the transmission slot waveguide 2; the third strip waveguide 6 and the fourth strip waveguide 7 opposite to each other are respectively arranged on both sides of the second transmission section, and the bottom surface of the third strip waveguide 6 is in line with the transmission slot waveguide 2 are flush with the bottom surface, and the top surface of the fourth strip waveguide 7 is flush with the top surface of the transmission slot waveguide 2; the first strip waveguide 4 and the third strip waveguide 6 are located on the same side of the transmission slot waveguide 2, and the second strip waveguide The strip waveguide 5 and the fourth strip waveguide 7 are located on the other side of the transmission slot waveguide 2 .

进一步的,所述槽波导由两根平行的硅基纳米线组成,两根硅基纳米线之间形成微槽。Further, the groove waveguide is composed of two parallel silicon-based nanowires, and a microgroove is formed between the two silicon-based nanowires.

进一步的,所述硅基纳米线的宽度为200nm,两根硅基纳米线之间的微槽宽度为100nm~120nm,第一至第四条形波导的长度为3.0μm~3.6μm。Further, the width of the silicon-based nanowires is 200nm, the width of the microgrooves between two silicon-based nanowires is 100nm-120nm, and the lengths of the first to fourth strip waveguides are 3.0μm-3.6μm.

进一步的,还包括衬底8和包层9,所述槽波导和第一至第四条形波导均设置在衬底8上并包裹在衬底8和包层9之间。Further, a substrate 8 and a cladding 9 are also included, and the slot waveguide and the first to fourth strip waveguides are all arranged on the substrate 8 and wrapped between the substrate 8 and the cladding 9 .

本发明还提出一种偏振旋转方法,该方法包括步骤:The present invention also proposes a polarization rotation method, the method comprising steps:

(a)构建如权利要求1至4所述的任意一项硅基双段式槽波导偏振旋转器;传输槽波导2的第一传输段、第一条形波导4和第二条形波导5构成第一偏振旋转区;传输槽波导2的第二传输段、第三条形波导6和第四条形波导7构成第二偏振旋转区;(a) construct any silicon-based double-section slot waveguide polarization rotator as claimed in claims 1 to 4; the first transmission section of the transmission slot waveguide 2, the first strip waveguide 4 and the second strip waveguide 5 Constitute the first polarization rotation region; the second transmission section of the transmission slot waveguide 2, the third strip waveguide 6 and the fourth strip waveguide 7 constitute the second polarization rotation region;

(b)将横磁模/横电模光信号从输入槽波导1输入,依次经过第一偏振旋转区和第二偏振旋转区;其中,第一偏振旋转区将输入光信号的光轴方向顺时针旋转角度形成第一次偏振旋转信号;第二偏振旋转区将第一次偏振旋转信号逆时针旋转角度形成光轴方向相对于初始输入的光信号逆时针旋转了角度的第二次偏振旋转信号并从输出槽波导3输出;若从输入槽波导1输入的信号为横磁模光信号,则输出槽波导3输出的信号为横电模光信号;若从输入槽波导1输入的信号为横电模光信号,则输出槽波导3输出的信号为横磁模光信号。(b) The transverse magnetic mode/transverse electric mode optical signal is input from the input groove waveguide 1, and passes through the first polarization rotation area and the second polarization rotation area in sequence; wherein, the first polarization rotation area changes the direction of the optical axis of the input optical signal along the Clock rotation angle Form the first polarization rotation signal; the second polarization rotation zone rotates the first polarization rotation signal counterclockwise The direction of the optical axis is rotated counterclockwise relative to the initial input optical signal The second polarization rotation signal of the output slot waveguide 3 is output from the output slot waveguide 3; if the signal input from the input slot waveguide 1 is a transverse magnetic mode optical signal, the signal output from the output slot waveguide 3 is a transverse electric mode optical signal; The signal input by the waveguide 1 is a transverse electric mode optical signal, and the signal output by the output slot waveguide 3 is a transverse magnetic mode optical signal.

进一步的,所述 Further, the

有益效果:Beneficial effect:

1、插入损耗低、偏振旋转效率高。本发明在槽波导的两侧按一上一下的方式加入了两个条形波导,并且在纵向引入了两段级联的波导结构(第二段中两条形波导的位置与第一段刚好相反)。由于所加入的条形波导的尺寸小,只用于改变模场光轴的方向,并且波导的长度短(单段仅为3.0μm~3.6μm),使得器件的插入损耗较低。此外通过双段结构的优化设计,可以实现输入偏振态在输出端90°的旋转,具有偏振旋转效率高的优点。1. Low insertion loss and high polarization rotation efficiency. The present invention adds two strip waveguides on both sides of the slot waveguide in an up-and-down manner, and introduces two sections of cascaded waveguide structures in the longitudinal direction (the positions of the two waveguides in the second section are exactly the same as those in the first section) on the contrary). Due to the small size of the added strip waveguide, it is only used to change the direction of the optical axis of the mode field, and the length of the waveguide is short (only 3.0 μm to 3.6 μm for a single section), so that the insertion loss of the device is low. In addition, through the optimized design of the double-segment structure, the input polarization state can be rotated by 90° at the output end, which has the advantage of high polarization rotation efficiency.

2、尺寸小、偏振旋转区长度短。如上所述,整个器件的偏振旋转区长度仅为6.0μm~7.2μm,利于实现器件的紧凑型设计和片上密集集成。2. Small size and short polarization rotation region length. As mentioned above, the length of the polarization rotation region of the entire device is only 6.0 μm to 7.2 μm, which is conducive to the realization of compact design and on-chip dense integration of the device.

3、器件制造相对容易。本发明器件的特征尺寸(最小尺寸)为100nm,即槽波导中间的微槽宽度,其完全兼容目前CMOS工艺线的尺寸许可,进而借助成熟的CMOS工艺线可以相对容易和高效地制造该器件。3. Device manufacturing is relatively easy. The feature size (minimum size) of the device of the present invention is 100nm, that is, the width of the microgroove in the middle of the groove waveguide, which is fully compatible with the size permit of the current CMOS process line, and the device can be manufactured relatively easily and efficiently with the help of a mature CMOS process line.

附图说明Description of drawings

图1为本发明实施例的结构示意图;Fig. 1 is the structural representation of the embodiment of the present invention;

图2为实施例中槽波导结构的横截面图;2 is a cross-sectional view of a slot waveguide structure in an embodiment;

图3为实施例中第一偏振旋转区结构的横截面图;3 is a cross-sectional view of the structure of the first polarization rotation region in the embodiment;

图4为实施例中第二偏振旋转区结构的横截面图;Fig. 4 is the cross-sectional view of the structure of the second polarization rotation region in the embodiment;

图5为实施例中偏振态光轴方向在经过第一偏振旋转区后的变化图;Fig. 5 is a change diagram of the polarization state optical axis direction after passing through the first polarization rotation region in the embodiment;

图6为实施例中偏振态光轴方向在经过第二偏振旋转区后的变化图;Fig. 6 is a change diagram of the polarization state optical axis direction after passing through the second polarization rotation region in the embodiment;

图7为实施例中器件的偏振旋转效率和插入损耗与工作波长的变化关系图。Fig. 7 is a graph showing the relationship between the polarization rotation efficiency and insertion loss of the device in the embodiment and the working wavelength.

图中:1、输入槽波导,2、传输槽波导,3、输出槽波导,4、第一条形波导,5、第二条形波导,6、第三条形波导,7、第四条形波导,8、衬底,9、包层。In the figure: 1. input slot waveguide, 2. transmission slot waveguide, 3. output slot waveguide, 4. first strip waveguide, 5. second strip waveguide, 6. third strip waveguide, 7. fourth strip waveguide Shaped waveguide, 8, substrate, 9, cladding.

具体实施方式detailed description

下面结合附图对本发明做更进一步的解释。The present invention will be further explained below in conjunction with the accompanying drawings.

如图1至图4所示为实施例一种硅基双段式槽波导偏振旋转器的结构图,它包括由两根硅基纳米线构成的槽波导和尺寸相同的第一条形波导4、第二条形波导5、第三条形波导6、和第四条形波导7;所述槽波导沿长度方向分为输入槽波导1、传输槽波导2和输出槽波导3;传输槽波导2沿长度方向均分为两段:第一传输段和第二传输段,其中,第一传输段两侧分别设有位置相对的第一条形波导4和第二条形波导5,第一条形波导4的顶面与传输槽波导2顶面相平齐,第二条形波导5的底面与传输槽波导2底面相平齐;第二传输段两侧分别设有位置相对的第三条形波导6和第四条形波导7,第三条形波导6的底面与传输槽波导2底面相平齐,第四条形波导7的顶面与传输槽波导2顶面相平齐;第一条形波导4和第三条形波导6位于传输槽波导2的同一侧,第二条形波导5和第四条形波导7位于传输槽波导2的另一侧。Figures 1 to 4 are structural diagrams of a silicon-based two-stage slot waveguide polarization rotator according to an embodiment, which includes a slot waveguide composed of two silicon-based nanowires and a first strip waveguide 4 of the same size. , the second strip waveguide 5, the third strip waveguide 6, and the fourth strip waveguide 7; the slot waveguide is divided into an input slot waveguide 1, a transmission slot waveguide 2 and an output slot waveguide 3 along the length direction; the transmission slot waveguide 2 divided into two sections along the length direction: the first transmission section and the second transmission section, wherein the first transmission section is respectively provided with a first strip waveguide 4 and a second strip waveguide 5 opposite to each other, and the first The top surface of the strip waveguide 4 is flush with the top surface of the transmission slot waveguide 2, and the bottom surface of the second strip waveguide 5 is flush with the bottom surface of the transmission slot waveguide 2; the two sides of the second transmission section are respectively provided with third strips opposite to each other. waveguide 6 and the fourth strip waveguide 7, the bottom surface of the third strip waveguide 6 is flush with the bottom surface of the transmission slot waveguide 2, and the top surface of the fourth strip waveguide 7 is flush with the top surface of the transmission slot waveguide 2; The strip waveguide 4 and the third strip waveguide 6 are located on the same side of the transmission slot waveguide 2 , and the second strip waveguide 5 and the fourth strip waveguide 7 are located on the other side of the transmission slot waveguide 2 .

在上述结构中,传输槽波导2的第一传输段、第一条形波导4和第二条形波导5构成第一偏振旋转区;传输槽波导2的第二传输段、第三条形波导6和第四条形波导7构成第二偏振旋转区。所述硅基纳米线的宽度为200nm,两根硅基纳米线之间的微槽宽度为100nm~120nm,第一至第四条形波导的长度为3.0μm~3.6μm。In the above structure, the first transmission section of the transmission slot waveguide 2, the first strip waveguide 4 and the second strip waveguide 5 constitute the first polarization rotation region; the second transmission section of the transmission slot waveguide 2, the third strip waveguide 6 and the fourth strip waveguide 7 constitute the second polarization rotation region. The width of the silicon-based nanowires is 200nm, the width of the microgrooves between two silicon-based nanowires is 100nm-120nm, and the lengths of the first to fourth strip waveguides are 3.0μm-3.6μm.

从输入槽波导1输入的横磁模光信号,在经过第一偏振旋转区和第二偏振旋转区后,在输出槽波导3输出端输出横电模的光信号;基于器件整体结构的中心对称特性,从输入槽波导1输入的横电模光信号,在经过第一和第二偏振旋转区后,在输出槽波导3输出端能够输出横磁模的光信号。The transverse magnetic mode optical signal input from the input slot waveguide 1, after passing through the first polarization rotation region and the second polarization rotation region, outputs the transverse electric mode optical signal at the output end of the output slot waveguide 3; based on the centrosymmetry of the overall structure of the device The characteristic is that the transverse electric mode optical signal input from the input slot waveguide 1 can output the transverse magnetic mode optical signal at the output end of the output slot waveguide 3 after passing through the first and second polarization rotation regions.

具体的,光信号在上述结构的硅基双段式槽波导偏振旋转器中的传输特征如下:取包含横磁模(TM)的入射光信号从输入槽波导1进入,接着进入传输槽波导2的第一偏振旋转区,因受到该旋转区中第一条形波导4和第二条形波导5的共同影响,输入的TM模光信号的偏振态光轴方向发生改变,在经过第一偏振旋转区后,相应的偏振态光轴方向改变了45°。接下来,光信号进入第二偏振旋转区,在该区域附加的条形波导的位置与第一偏振旋转区的刚好相反,即第三条形波导6和第四条形波导7,因受结构垂直和水平非对称的影响,光信号的模式将进一步发生旋转,并从输出槽波导3进行输出。所以在输出端可以获得90°的偏振旋转角,对应于横电模(TE)的输出光信号,从而实现了偏振旋转的功能。这种旋转器的结构简单,其原理可以通过简单的偏振态光轴方向的变化进行分析,如图5、6所示,其中第一/二偏振旋转区的模式光轴方向与水平/垂直方向的夹角为(通过优化槽波导两侧条形波导的尺寸,进而可改变偏振旋转区模式光轴的方向,以实现所需夹角值其中模式的计算采用数值模式求解器)。输入的TM模光信号在经过第一偏振旋转区后,偏振角顺时针旋转了接着在经过第二旋转区后,由于本征模的光轴方向发生了变化(逆向旋转了),导致偏振角逆时针旋转了相对于初始TM模净旋转了若要实现90°的偏振态旋转,即这也是偏振旋转区两条形波导尺寸优化的目标(使得偏振旋转区本征模的光轴与水平或者垂直方向的夹角为22.5°)。与传统的单段式偏振旋转器相比,本发明通过引入双段式偏振耦合区结构,理论上在输出端可以输出包含任意偏振旋转角(0~90°之间)的光信号模式,可用于设计紧凑型片上光学波片。考虑到实际情况,针对槽波导,本实施例中,我们只输出TE模光信号,对应于实现90°的偏振旋转角,此外该器件具有较小的插入损耗和较高的偏振旋转效率,可应用于片上紧凑型槽波导器件的偏振控制。Specifically, the transmission characteristics of the optical signal in the silicon-based two-stage slot waveguide polarization rotator with the above structure are as follows: The incident optical signal containing the transverse magnetic mode (TM) enters from the input slot waveguide 1, and then enters the first polarization rotation region of the transmission slot waveguide 2, due to being subjected to the first polarization rotation region in the rotation region, the first strip waveguide 4 and the second strip waveguide 5 Due to the common influence of the input TM mode optical signal, the direction of the polarization axis of the optical signal changes, and after passing through the first polarization rotation region, the direction of the corresponding polarization axis changes by 45°. Next, the optical signal enters the second polarization rotation region, where the additional strip waveguides are located just opposite to those in the first polarization rotation region, that is, the third strip waveguide 6 and the fourth strip waveguide 7, due to the structure Due to the influence of vertical and horizontal asymmetry, the mode of the optical signal will be further rotated and output from the output slot waveguide 3 . Therefore, a polarization rotation angle of 90° can be obtained at the output end, corresponding to the output optical signal of the transverse electric mode (TE), thereby realizing the function of polarization rotation. The structure of this rotator is simple, and its principle can be analyzed by simply changing the direction of the polarization axis, as shown in Figures 5 and 6, where the direction of the mode axis of the first/second polarization rotation zone is different from the horizontal/vertical direction The included angle is (By optimizing the size of the strip waveguide on both sides of the groove waveguide, the direction of the optical axis of the polarization rotation zone mode can be changed to achieve the required angle value where the model is computed using a numerical model solver). After the input TM mode optical signal passes through the first polarization rotation region, the polarization angle rotates clockwise Then after passing through the second rotation zone, due to the change of the optical axis direction of the eigenmode (reverse rotation ), causing the polarization angle to rotate counterclockwise A net rotation relative to the initial TM To achieve a 90° polarization state rotation, that is but This is also the goal of optimizing the dimensions of the two-shaped waveguide in the polarization rotation region (so that the angle between the optical axis of the eigenmode in the polarization rotation region and the horizontal or vertical direction is 22.5°). Compared with the traditional single-segment polarization rotator, the present invention introduces a double-segment polarization coupling region structure, which can theoretically output an optical signal mode containing any polarization rotation angle (between 0° and 90°) at the output end, which can be used For designing compact on-chip optical waveplates. Considering the actual situation, for the slot waveguide, in this embodiment, we only output the TE mode optical signal, which corresponds to realizing a polarization rotation angle of 90°. In addition, the device has a small insertion loss and a high polarization rotation efficiency, which can be Polarization control for on-chip compact slot waveguide devices.

图2为本实施例中槽波导的横截面图,形成槽波导的两根硅基纳米线(宽度约为200nm)被中间的微槽隔开,微槽的宽度为100nm~120nm,基于电场的边值关系,模场将在该微槽中出现显著的增强效应,对应于槽波导的场增强模式,也就是本发明所设计的偏振旋转器的输出模式。图3为第一偏振旋转区波导的横截面图,第一、第二条形波导分别位于构成槽波导的两硅基纳米线的两侧,按一上一下的方式排列。在槽波导的基础上借助两条形波导,可以打破原始结构的对称性,通过进一步优化设计条形波导的尺寸,在输出端可以获得所需光轴角对应的偏振态模式。图4为第二偏振旋转区波导的横截面图,其结构与第一偏振旋转区类似,差别仅在于两侧条形波导的排列方式发生了上下颠倒,以此来改变其本征模的光轴方向(如图5、6所示),进而改变传输光信号的偏振态光轴方向。Figure 2 is a cross-sectional view of the slot waveguide in this embodiment. Two silicon-based nanowires (about 200 nm in width) forming the slot waveguide are separated by a microgroove in the middle, and the width of the microgroove is 100 nm to 120 nm. Boundary value relationship, the mode field will have a significant enhancement effect in the microgroove, corresponding to the field enhancement mode of the groove waveguide, that is, the output mode of the polarization rotator designed in the present invention. Fig. 3 is a cross-sectional view of the waveguide in the first polarization rotation region. The first and second strip waveguides are respectively located on both sides of the two silicon-based nanowires forming the slot waveguide, arranged one above the other. The symmetry of the original structure can be broken by using two waveguides on the basis of the slot waveguide. By further optimizing the size of the strip waveguide, the polarization mode corresponding to the required optical axis angle can be obtained at the output end. Figure 4 is a cross-sectional view of the waveguide in the second polarization rotation region. Its structure is similar to that of the first polarization rotation region. The only difference is that the arrangement of the strip waveguides on both sides is upside down, so as to change the light of its eigenmode. axis direction (as shown in Figures 5 and 6), and then change the polarization state optical axis direction of the transmitted optical signal.

图7为本实施例中硅基双段式槽波导偏振旋转器的偏振旋转效率、插入损耗与工作波长的变化关系。从图中可以看出,该器件的工作带宽较大,当工作波长位于1.45μm~1.64μm时,偏振旋转效率始终大于90%,特别是在1.55μm处,偏振旋转效率更是高于97.5%。同时,插入损耗在计算波长范围内均小于0.4dB,表现出较好的频谱特性。由于硅基双段式槽波导偏振旋转器是中心对称结构,对于输入TE模的光信号,在经过第一和第二偏振旋转区之后,在输出端也能够输出TM模的光信号。此外,通过在第一或者第二偏振旋转区添加有源控制结构,可以适当的调节偏振旋转角,进而在输出端可以获得基于偏振态的光调制器或者光开关。最后,本发明所提供的双段式槽波导偏振旋转器方案,也可以用于设计其它类型波导结构(如硅基纳米线、混合等离子波导、光子晶体波导等)的偏振旋转器。FIG. 7 shows the relationship between the polarization rotation efficiency, insertion loss and working wavelength of the silicon-based double-stage slot waveguide polarization rotator in this embodiment. It can be seen from the figure that the device has a large working bandwidth. When the working wavelength is between 1.45 μm and 1.64 μm, the polarization rotation efficiency is always greater than 90%, especially at 1.55 μm, the polarization rotation efficiency is even higher than 97.5%. . At the same time, the insertion loss is less than 0.4dB in the calculated wavelength range, showing better spectral characteristics. Since the silicon-based double-segment slot waveguide polarization rotator has a centrosymmetric structure, the input TE mode optical signal can also output the TM mode optical signal at the output end after passing through the first and second polarization rotation regions. In addition, by adding an active control structure in the first or second polarization rotation region, the polarization rotation angle can be properly adjusted, and then an optical modulator or optical switch based on the polarization state can be obtained at the output end. Finally, the dual-stage slot waveguide polarization rotator solution provided by the present invention can also be used to design polarization rotators for other types of waveguide structures (such as silicon-based nanowires, hybrid plasmonic waveguides, photonic crystal waveguides, etc.).

以上所述仅是本发明的优选实施方式,应当指出,对于本技术领域的普通技术人员来说,在不脱离本发明原理的前提下,还可以做出若干改进和润饰,这些改进和润饰也应视为本发明的保护范围。The above is only a preferred embodiment of the present invention, it should be pointed out that, for those of ordinary skill in the art, without departing from the principle of the present invention, some improvements and modifications can also be made, and these improvements and modifications can also be made. It should be regarded as the protection scope of the present invention.

Claims (6)

1. a silica-based two section type groove waveguides polarization rotator, it is characterised in that include groove waveguides and equivalently-sized first to fourth slab waveguide (4,5,6,7);Described groove waveguides is divided into input slot waveguide (1), transmission slot waveguide (2) and output magazine waveguide (3) along its length;Transmission slot waveguide (2) is divided into the two sections: first span line and the second span line along its length, wherein, first span line is respectively provided on two sides with relative the first slab waveguide (4) in position and the second slab waveguide (5), the end face of the first slab waveguide (4) and transmission slot waveguide (2) end face flush, the bottom surface of the second slab waveguide (5) and transmission slot waveguide (2) bottom surface flush;Second span line is respectively provided on two sides with relative Article 3 shape waveguide (6) in position and Article 4 shape waveguide (7), the bottom surface of Article 3 shape waveguide (6) and transmission slot waveguide (2) bottom surface flush, the end face of Article 4 shape waveguide (7) and transmission slot waveguide (2) end face flush;First slab waveguide (4) and Article 3 shape waveguide (6) are positioned at the same side of transmission slot waveguide (2), the second slab waveguide (5) and Article 4 shape waveguide (7) and are positioned at the opposite side of transmission slot waveguide (2).
2. the silica-based two section type groove waveguides polarization rotator of one according to claim 1, it is characterised in that described groove waveguides is made up of two parallel silica-based nanowires, forms microflute between two silica-based nanowires.
3. the silica-based two section type groove waveguides polarization rotator of one according to claim 2, it is characterized in that, the width of described silica-based nanowire is 200nm, width of mini longitudinal channels between two silica-based nanowires is 100nm~120nm, first to fourth slab waveguide (4,5,6,7) length is 3.0 μm~3.6 μm.
4. the silica-based two section type groove waveguides polarization rotator of one according to claim 1, it is characterized in that, also include substrate (8) and covering (9), described groove waveguides and first to fourth slab waveguide (4,5,6,7) it is arranged at substrate (8) above and to be wrapped between substrate (8) and covering (9).
5. a polarization spinning solution, it is characterised in that include step:
A () builds the silica-based two section type groove waveguides polarization rotator of any one as described in Claims 1-4;First span line of transmission slot waveguide (2), the first slab waveguide (4) and the second slab waveguide (5) constitute the first polarization Rotary District;Second span line of transmission slot waveguide (2), Article 3 shape waveguide (6) and Article 4 shape waveguide (7) constitute the second polarization Rotary District;
B TM mode/transverse electric mode optical signal is inputted by () from input slot waveguide (1), sequentially pass through the first polarization Rotary District and the second polarization Rotary District;Wherein, the first polarization Rotary District is by the optical axis direction dextrorotation gyration of input optical signalFormed and polarize rotating signal for the first time;Second polarization Rotary District is by first time polarization rotating signal rotated counterclockwise by angleForm optical axis direction and have rotated angle counterclockwise relative to the optical signal of initial inputSecond time polarization rotating signal and from output magazine waveguide (3) export;If the signal inputted from input slot waveguide (1) is TM mode optical signal, then the signal that output magazine waveguide (3) exports is transverse electric mode optical signal;If the signal inputted from input slot waveguide (1) is transverse electric mode optical signal, then the signal that output magazine waveguide (3) exports is TM mode optical signal.
6. a kind of polarization spinning solution according to claim 5, it is characterised in that described in
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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109188599A (en) * 2018-10-30 2019-01-11 西安邮电大学 A kind of dual-trench type big negative dispersion waveguide in 1530nm to 1580nm wavelength band
CN109417271A (en) * 2016-07-27 2019-03-01 英特尔公司 The closed loop on piece isolator of feedback control
CN111474629A (en) * 2020-04-08 2020-07-31 浙江西湖高等研究院 A kind of polarization rotation beam splitter based on strip geometry waveguide and its preparation method
US20220373738A1 (en) * 2021-05-24 2022-11-24 Globalfoundries U.S. Inc. Switchable polarization rotators

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101320113A (en) * 2008-07-15 2008-12-10 浙江大学 A Waveguide Polarization Mode Converter
CN103336330A (en) * 2013-07-05 2013-10-02 中国科学院半导体研究所 Polarization rotator based on asymmetric vertical slot waveguide
CN103558661A (en) * 2013-11-11 2014-02-05 东南大学 Integrated polarization converter based on silicon-based L-shaped waveguide structure
US20150003782A1 (en) * 2013-06-27 2015-01-01 Fujikura Ltd. Polarization conversion device
CN105319644A (en) * 2014-07-04 2016-02-10 中国科学院苏州纳米技术与纳米仿生研究所 Waveguide-type polarization converter and preparation method thereof
CN105572800A (en) * 2016-01-26 2016-05-11 东南大学 Polarization rotator based on silicon-on-insulator waveguide coupling

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101320113A (en) * 2008-07-15 2008-12-10 浙江大学 A Waveguide Polarization Mode Converter
US20150003782A1 (en) * 2013-06-27 2015-01-01 Fujikura Ltd. Polarization conversion device
CN103336330A (en) * 2013-07-05 2013-10-02 中国科学院半导体研究所 Polarization rotator based on asymmetric vertical slot waveguide
CN103558661A (en) * 2013-11-11 2014-02-05 东南大学 Integrated polarization converter based on silicon-based L-shaped waveguide structure
CN105319644A (en) * 2014-07-04 2016-02-10 中国科学院苏州纳米技术与纳米仿生研究所 Waveguide-type polarization converter and preparation method thereof
CN105572800A (en) * 2016-01-26 2016-05-11 东南大学 Polarization rotator based on silicon-on-insulator waveguide coupling

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
王嘉源 等: "硅基槽波导级联多模干涉耦合器型偏振分束器", 《红外与毫米波学报》 *

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109417271A (en) * 2016-07-27 2019-03-01 英特尔公司 The closed loop on piece isolator of feedback control
CN109188599A (en) * 2018-10-30 2019-01-11 西安邮电大学 A kind of dual-trench type big negative dispersion waveguide in 1530nm to 1580nm wavelength band
CN111474629A (en) * 2020-04-08 2020-07-31 浙江西湖高等研究院 A kind of polarization rotation beam splitter based on strip geometry waveguide and its preparation method
CN111474629B (en) * 2020-04-08 2022-07-15 浙江西湖高等研究院 Polarization rotation beam splitter based on strip-shaped geometric waveguide and preparation method thereof
US20220373738A1 (en) * 2021-05-24 2022-11-24 Globalfoundries U.S. Inc. Switchable polarization rotators
US11644620B2 (en) * 2021-05-24 2023-05-09 Globalfoundries U.S. Inc. Switchable polarization rotators

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