CN103901559B - Optical coupling device - Google Patents
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Abstract
Description
技术领域technical field
本发明涉及集成光学装置,特别涉及一种光耦合装置。The invention relates to an integrated optical device, in particular to an optical coupling device.
背景技术Background technique
集成光学中普遍采用方向性较佳的激光作为光源,然而激光发出的光束仍具有一定的发散角,如果直接让光源与光学元件对接,光束中的发散光线将无法进入光学元件,光利用率低。因此,如何将光源耦合至光学元件以使发散的光束汇聚入光学元件以提高光利用率是一个重要课题。In integrated optics, laser light with better directionality is generally used as the light source. However, the beam emitted by the laser still has a certain divergence angle. If the light source is directly connected to the optical element, the divergent light in the beam will not be able to enter the optical element, and the light utilization rate will be low. . Therefore, how to couple the light source to the optical element so that the divergent light beam converges into the optical element to improve light utilization is an important issue.
发明内容Contents of the invention
有鉴于此,有必要提供一种能够提高光利用率的光耦合装置。In view of this, it is necessary to provide an optical coupling device capable of improving light utilization.
一种光耦合装置,其包括一个基底、一个形成于所述基底上的平板光波导及一个形成于所述平板光波导上的介质光栅薄膜。所述平板光波导用于与一个激光光源对接以接收所述激光光源发出的发散的激光束,所述介质光栅薄膜包括一个第一介质光栅及一个与所述第一介质光栅间隔设置的第二介质光栅。所述第一介质光栅位于所述激光光源的出射光路并用于将所述发散的激光束汇聚为平行的激光束。所述第二介质光栅位于所述第一介质光栅的出射光路并用于汇聚所述平行激光束并将汇聚的所述平行光束耦合至一光学元件。An optical coupling device includes a substrate, a flat optical waveguide formed on the substrate, and a dielectric grating film formed on the flat optical waveguide. The slab optical waveguide is used for docking with a laser light source to receive the divergent laser beam emitted by the laser light source, and the dielectric grating film includes a first dielectric grating and a second dielectric grating spaced apart from the first dielectric grating. Media grating. The first dielectric grating is located on the exit light path of the laser light source and is used to converge the diverging laser beams into parallel laser beams. The second dielectric grating is located on the outgoing light path of the first dielectric grating and is used for converging the parallel laser beams and coupling the collimated parallel beams to an optical element.
根据集成光学理论,所述第一介质光栅及第二介质光栅例如均设置成啁啾光栅(chirped grating),进一步根据所述激光光源与光学元件之间的相对位置,合理设置第一介质光栅及第二介质光栅的结构从而使激光光源发出的激光束耦合至所述光学元件。According to the theory of integrated optics, for example, the first dielectric grating and the second dielectric grating are set as chirped gratings, and further according to the relative position between the laser light source and the optical element, the first dielectric grating and the second dielectric grating are set reasonably. The structure of the second dielectric grating is such that the laser beam emitted by the laser light source is coupled to the optical element.
附图说明Description of drawings
图1为本发明提供的光耦合装置的结构示意图。FIG. 1 is a schematic structural diagram of an optical coupling device provided by the present invention.
图2为图1的光耦合装置沿线II-II的剖面示意图。FIG. 2 is a schematic cross-sectional view of the optical coupling device of FIG. 1 along the line II-II.
图3为图1中的第一介质光栅的平面示意图。FIG. 3 is a schematic plan view of the first dielectric grating in FIG. 1 .
主要元件符号说明Explanation of main component symbols
光耦合装置 10Optocoupler 10
基底 110base 110
顶面 111top 111
侧面 112side 112
平板光波导 120Planar optical waveguide 120
介质光栅薄膜 130Dielectric Grating Film 130
第一介质光栅 131First dielectric grating 131
第一矩形凸条 1311First rectangular rib 1311
第二矩形凸条 1312Second rectangular rib 1312
第一对称轴 OFirst axis of symmetry O
第二介质光栅 132Second dielectric grating 132
第三矩形凸条 1321Third rectangular rib 1321
第四矩形凸条 1322Fourth rectangular rib 1322
第二对称轴 ASecond axis of symmetry A
矩形凹槽 133Rectangular groove 133
激光光源 20Laser light source 20
激光束 21laser beam 21
光学元件 30Optics 30
如下具体实施方式将结合上述附图进一步说明本发明。The following specific embodiments will further illustrate the present invention in conjunction with the above-mentioned drawings.
具体实施方式detailed description
下面将结合附图对本发明实施方式作进一步的详细说明。The embodiments of the present invention will be further described in detail below in conjunction with the accompanying drawings.
请参阅图1及图2,本发明实施方式提供的光耦合装置10包括一个基底110、一个形成于所述基底110上的平板光波导120及一个形成于所述平板光波导120上的介质光栅薄膜130。1 and 2, the optical coupling device 10 provided by the embodiment of the present invention includes a substrate 110, a slab optical waveguide 120 formed on the substrate 110, and a dielectric grating formed on the slab optical waveguide 120. Film 130.
所述基底110基本呈矩形,并包括一个顶面111及一个与所述顶面111垂直连接的侧面112。考虑到铌酸锂扩散金属钛(单质)可以形成折射率渐变型的加载光波导,因此,所述基底110的材料采用铌酸锂晶体。在其他实施方式中,所述基底110也可以是陶瓷或塑料等材料,通过半导体制程在陶瓷或塑料的基底110上形成半导体材料如二氧化硅、硅等材料从而形成的所述平板光波导120。The base 110 is substantially rectangular and includes a top surface 111 and a side surface 112 vertically connected to the top surface 111 . Considering that lithium niobate diffused metal titanium (single substance) can form a loaded optical waveguide with graded refractive index, the material of the substrate 110 is lithium niobate crystal. In other embodiments, the substrate 110 may also be made of materials such as ceramics or plastics, and the planar optical waveguide 120 is formed by forming semiconductor materials such as silicon dioxide, silicon, and other materials on the ceramic or plastic substrate 110 through a semiconductor process. .
所述平板光波导120通过向所述顶面111镀上金属钛后高温将金属钛扩散入所述基底110而形成。在本实施方式中,对应所述基底110的形状,所述平板光波导120为矩形,所述顶面111即为所述平板光波导120的顶面,所述侧面112即为所述平板光波导120的侧面。所述平板光波导120用于与一个激光光源20对接以接收所述激光光源20发出的激光束21。The planar optical waveguide 120 is formed by coating the top surface 111 with titanium metal and then diffusing the titanium metal into the base 110 at high temperature. In this embodiment, corresponding to the shape of the substrate 110, the flat optical waveguide 120 is rectangular, the top surface 111 is the top surface of the flat optical waveguide 120, and the side surface 112 is the flat optical waveguide 120. side of the waveguide 120 . The flat optical waveguide 120 is used to connect with a laser light source 20 to receive the laser beam 21 emitted by the laser light source 20 .
所述介质光栅薄膜130通过在所述顶面111上通过溅射镀膜、蒸镀或涂布一层高折射率材料膜而形成,所述高折射率材料可二氧化硅、二氧化硅掺硼或磷的混合物或有机化合物。本实施方式中,所述介质光栅薄膜130为涂布于所述顶面111上的有机化合物,且通过在所述有机化合物的介质光栅薄膜130上采用黄光蚀刻(黄光微影)工艺蚀刻从而形成一个第一介质光栅131及一个与所述第一介质光栅间隔设置的第二介质光栅132。The dielectric grating film 130 is formed by sputtering, evaporating or coating a layer of high refractive index material film on the top surface 111, and the high refractive index material can be silicon dioxide, silicon dioxide doped with boron or mixtures of phosphorus or organic compounds. In this embodiment, the dielectric grating film 130 is an organic compound coated on the top surface 111, and is formed by etching the dielectric grating film 130 of the organic compound using a yellow photolithography (yellow photolithography) process. A first dielectric grating 131 and a second dielectric grating 132 spaced apart from the first dielectric grating.
本实施方式中,所述第一介质光栅131为一个啁啾光栅。所述第一介质光栅131包括一个位于中间的第一矩形凸条1311及多个对称分布于所述第一矩形凸条1311两侧的第二矩形凸条1312,所述第一矩形凸条1311及所述第二矩形凸条1312的数量之和为奇数,所述第一矩形凸条1311与多个第二矩形凸条1312互相平行间隔设置,所述第一矩形凸条1311的宽度大于每个第二矩形凸条1312的宽度,且从所述第一矩形凸条1311到远离所述第一矩形凸条1311的方向,所述多个第二矩形凸条1312的宽度越来越小,而所述第二矩形凸条1312与第一矩形凸条1311及相邻两个第二矩形凸条1312之间的间隙也越来越小。In this implementation manner, the first dielectric grating 131 is a chirped grating. The first dielectric grating 131 includes a first rectangular convex strip 1311 in the middle and a plurality of second rectangular convex strips 1312 symmetrically distributed on both sides of the first rectangular convex strip 1311. The first rectangular convex strip 1311 And the sum of the number of the second rectangular convex strips 1312 is an odd number, the first rectangular convex strips 1311 and a plurality of second rectangular convex strips 1312 are arranged in parallel with each other, and the width of the first rectangular convex strips 1311 is greater than each The width of each second rectangular convex strip 1312, and from the first rectangular convex strip 1311 to the direction away from the first rectangular convex strip 1311, the width of the plurality of second rectangular convex strips 1312 becomes smaller and smaller, And the gaps between the second rectangular convex strip 1312 and the first rectangular convex strip 1311 and two adjacent second rectangular convex strips 1312 are getting smaller and smaller.
请参阅图3,本实施方式中,所述第一矩形凸条1311包括一个与所述平板光波导120相背的矩形上表面。该第一矩形凸条1311的矩形上表面包括两条长边及两条宽边。以所述第一矩形凸条1311的矩形上表面的两条宽边的中心点的连线作为第一对称轴O,所述第一介质光栅131的的矩形上表面的其中一条宽边的延伸方向为x轴,所述第一对称轴O于x轴的相交点为原点,沿所述第一对称轴O到远离所述第一对称轴O的方向为x轴正向,以所述激光束21在x处与原点处的相位差为y轴,根据平板光波导波动理论可得:其中x>0,则所述第一介质光栅131的第n个边界xn满足如下条件:其中,n为正整数,yn=nπ,a及k为常数与衍射型光波导透镜的焦距相关。如此,可推得:而x<0的情况,即所述第一对称轴O左边的所述第一介质光栅1311的边界可通过对称性获得。Please refer to FIG. 3 , in this embodiment, the first rectangular convex strip 1311 includes a rectangular upper surface opposite to the planar optical waveguide 120 . The rectangular upper surface of the first rectangular protrusion 1311 includes two long sides and two wide sides. Taking the line connecting the central points of the two broad sides of the rectangular upper surface of the first rectangular convex strip 1311 as the first axis of symmetry O, the extension of one of the broad sides of the rectangular upper surface of the first dielectric grating 131 The direction is the x-axis, the intersection point of the first symmetry axis O on the x-axis is the origin, the direction along the first symmetry axis O to the direction away from the first symmetry axis O is the positive direction of the x-axis, and the laser The phase difference between the beam 21 at x and the origin is the y axis, and according to the planar optical waveguide wave theory: Where x>0, then the nth boundary x n of the first dielectric grating 131 satisfies the following conditions: Wherein, n is a positive integer, y n =nπ, and a and k are constants related to the focal length of the diffractive optical waveguide lens. In this way, it can be deduced that: In the case of x<0, that is, the boundary of the first dielectric grating 1311 on the left side of the first symmetry axis O can be obtained through symmetry.
请再次参阅图1,所述第二介质光栅132结构与所述第一介质光栅131的结构完全相同,也为一个啁啾光栅且关于一个第二对称轴A对称。所述第二介质光栅132包括一个位于中间的第三矩形凸条1321及多个对称分布于所述第三矩形凸条1321两侧的第四矩形凸条1322,所述第三矩形凸条1321及所述第四矩形凸条1322的数量之和为奇数,所述第三矩形凸条1321与多个第四矩形凸条1322互相平行间隔设置,所述第三矩形凸条1321的宽度大于每个第四矩形凸条1322的宽度,且从所述第三矩形凸条1321到远离所述第三矩形凸条1321的方向,所述多个第四矩形凸条1322的宽度越来越小,而所述第四矩形凸条1322与第三矩形凸条1321及相邻两个第四矩形凸条1322之间的间隙也越来越小。Please refer to FIG. 1 again, the structure of the second dielectric grating 132 is exactly the same as that of the first dielectric grating 131 , it is also a chirped grating and is symmetrical about a second symmetry axis A. The second dielectric grating 132 includes a third rectangular convex strip 1321 in the middle and a plurality of fourth rectangular convex strips 1322 symmetrically distributed on both sides of the third rectangular convex strip 1321. The third rectangular convex strip 1321 And the sum of the number of the fourth rectangular convex strips 1322 is an odd number, the third rectangular convex strips 1321 and a plurality of fourth rectangular convex strips 1322 are arranged in parallel with each other, and the width of the third rectangular convex strips 1321 is greater than each The width of each fourth rectangular convex strip 1322, and from the third rectangular convex strip 1321 to the direction away from the third rectangular convex strip 1321, the width of the plurality of fourth rectangular convex strips 1322 becomes smaller and smaller, And the gaps between the fourth rectangular convex strip 1322 and the third rectangular convex strip 1321 and two adjacent fourth rectangular convex strips 1322 are getting smaller and smaller.
所述第一介质光栅131及所述第二介质光栅132之间开设有一个矩形凹槽133。所述矩形凹槽133的宽度即所述第一介质光栅131与所述第二介质光栅132之间的距离。所述第一对称轴O对准所述第二对称轴A。每一个第二矩形凸条1312对准对应一个第四矩形凸条1322。A rectangular groove 133 is defined between the first dielectric grating 131 and the second dielectric grating 132 . The width of the rectangular groove 133 is the distance between the first dielectric grating 131 and the second dielectric grating 132 . The first axis of symmetry O is aligned with the second axis of symmetry A. Each second rectangular protruding strip 1312 corresponds to a fourth rectangular protruding strip 1322 .
所述激光光源20采用分布式反馈激光器(distributed feedback laser,DFB),其属于侧面发射的半导体激光器,可以通过芯片焊接(die bond)方式将发光的侧面直接焊接到所述侧面112上,且所述激光光源20的中心轴对准所述第一对称轴O入射。当然,所述激光光源20也可以采用其他类型激光光源,并通过其他方式设置。所述第一介质光栅131位于所述激光光源的出射光路。所述第二介质光栅132位所述第一介质光栅131的出射光路。The laser light source 20 adopts a distributed feedback laser (distributed feedback laser, DFB), which belongs to a side-emitting semiconductor laser, and the light-emitting side can be directly welded to the side 112 by a die bond method, and the The central axis of the laser light source 20 is incident on the first axis of symmetry O. Certainly, the laser light source 20 may also adopt other types of laser light sources and be arranged in other ways. The first dielectric grating 131 is located in the outgoing light path of the laser light source. The second dielectric grating 132 is located in the outgoing optical path of the first dielectric grating 131 .
所述光耦合装置10还进一步包括一设置于所述第二介质光栅132的出光光路上的光学元件30所述,所述光学元件30的中心轴对准所述第三矩形凸条1321的中心轴,如此所述第一矩形凸条1311、所述第二矩形凸条1312、所述第三矩形凸条1321及所述第四矩形凸条1322均平行于所述激光光源20及所述光学元件30的中心轴的连线设置。所述光学元件30可以为条状光波导、光纤或者分光器(splitter)。本实施方式中,所述光学元件30为条状光波导。The optical coupling device 10 further includes an optical element 30 arranged on the light-emitting optical path of the second dielectric grating 132, the central axis of the optical element 30 is aligned with the center of the third rectangular convex strip 1321 axis, so that the first rectangular convex strip 1311, the second rectangular convex strip 1312, the third rectangular convex strip 1321 and the fourth rectangular convex strip 1322 are all parallel to the laser light source 20 and the optical The connecting line of the central axis of the element 30 is set. The optical element 30 may be a strip optical waveguide, an optical fiber or a splitter. In this embodiment, the optical element 30 is a strip optical waveguide.
使用时,所述激光光源20发出发散的激光束并将发散的激光束投向所述第一介质光栅131。所述第一介质光栅131将所述发散的激光束汇聚为平行的激光束。所述第二介质光栅132位汇聚所述平行激光束并将汇聚的所述平行光束耦合至所述光学元件30。In use, the laser light source 20 emits divergent laser beams and projects the divergent laser beams to the first dielectric grating 131 . The first dielectric grating 131 converges the diverging laser beams into parallel laser beams. The second dielectric grating 132 condenses the parallel laser beams and couples the condensed parallel beams to the optical element 30 .
根据集成光学理论,根据所述激光光源20与光学元件30之间的相对位置,合理设置第一介质光栅131及第二介质光栅132的结构、所述第一介质光栅131相对于激光光源20的位置以及第二介质光栅132相对于所述光学元件30的位置,从而使激光光源20发出的激光束耦合至所述光学元件30。According to the theory of integrated optics, according to the relative position between the laser light source 20 and the optical element 30, the structure of the first dielectric grating 131 and the second dielectric grating 132, and the structure of the first dielectric grating 131 relative to the laser light source 20 are reasonably set. position and the position of the second dielectric grating 132 relative to the optical element 30 , so that the laser beam emitted by the laser light source 20 is coupled to the optical element 30 .
虽然本发明已以较佳实施方式披露如上,但是,其并非用以限定本发明,另外,本领域技术人员还可以在本发明精神内做其它变化等。当然,这些依据本发明精神所做的变化,都应包含在本发明所要求保护的范围之内。Although the present invention has been disclosed above with preferred embodiments, it is not intended to limit the present invention. In addition, those skilled in the art can also make other changes within the spirit of the present invention. Of course, these changes made according to the spirit of the present invention should all be included within the scope of protection claimed by the present invention.
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