CN101825743A - Fluid optical waveguide structure - Google Patents

Fluid optical waveguide structure Download PDF

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CN101825743A
CN101825743A CN 201010128851 CN201010128851A CN101825743A CN 101825743 A CN101825743 A CN 101825743A CN 201010128851 CN201010128851 CN 201010128851 CN 201010128851 A CN201010128851 A CN 201010128851A CN 101825743 A CN101825743 A CN 101825743A
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substrate
optical waveguide
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metal electrode
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CN101825743B (en
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黎永前
丁丽娟
王宁博
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NANTONG JINNIU MACHINERY MANUFACTURE CO Ltd
Northwestern Polytechnical University
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Abstract

本发明公开了一种流体光波导的结构,其基于流体折射率随温度变化而变化的原理,采用电极加热的方法形成流体光波导。依次包括基底I、结构层和基底II。结构层上有微管道,其两端分别与输入口5和输出口7连通。一对金属电极分别处在基底I和基底II相应的位置上,或者处在结构层的两个内壁上,或者包覆整个微管道。基底I上与结构层上输入口5和输出口7相应的位置上布有开孔。为了保证金属电极和流体绝缘,可以在金属电极上覆盖聚合物薄膜。由于可以使用任意同种流体,使得流体光波导的材料选择性更灵活;通过简单电路控制,实现光在流体光波导中稳定传播,为生物细胞及生物大分子的光学检测提供了简便工具。

The invention discloses a structure of a fluid optical waveguide, which is based on the principle that the refractive index of the fluid changes with temperature, and adopts an electrode heating method to form the fluid optical waveguide. Substrate I, structural layer and substrate II are sequentially included. There is a micropipe on the structural layer, and its two ends communicate with the input port 5 and the output port 7 respectively. A pair of metal electrodes are respectively located on the corresponding positions of the base I and the base II, or are located on the two inner walls of the structural layer, or cover the entire micropipe. Openings are arranged on the substrate 1 at positions corresponding to the input port 5 and the output port 7 on the structural layer. In order to ensure the insulation between the metal electrode and the fluid, a polymer film can be covered on the metal electrode. Since any same fluid can be used, the material selection of the fluid optical waveguide is more flexible; through simple circuit control, the stable propagation of light in the fluid optical waveguide is realized, which provides a simple tool for the optical detection of biological cells and biological macromolecules.

Description

流体光波导结构 Fluid optical waveguide structure

所属领域Field

本发明涉及一种流体光波导结构,属于微机械电子系统(MEMS)、集成光学领域的流体光波导领域。The invention relates to a fluid optical waveguide structure, which belongs to the field of fluid optical waveguides in the field of micromechanical electronic systems (MEMS) and integrated optics.

现有技术current technology

流体光波导能够为生物检测提供赖于生存的液体环境,同时提供光信息传输的物理通道,近年来得到了广泛的研究。目前研究中的流体光波导的结构包括三种:(1)导波层材料为流体,覆盖层材料为固体;(2)导波层材料为流体,覆盖层材料为流体;(3)导波层材料为流体,覆盖层材料为气体。Fluid optical waveguides can provide a living liquid environment for biological detection, and at the same time provide a physical channel for optical information transmission, and have been extensively studied in recent years. The structure of the fluid optical waveguide in the current research includes three types: (1) the material of the waveguide layer is fluid, and the material of the cladding layer is solid; (2) the material of the waveguide layer is fluid, and the material of the cladding layer is fluid; (3) the guide wave The layer material is a fluid and the cover layer material is a gas.

由流体导波层和固体覆盖层构成的流体光波导。中国专利(CN200710044173.3)中提出了一种由流体导波层和固体覆盖层构成的流体光波导结构,选择折射率大于固体覆盖层折射率的流体,使得光在流体导波层发生全内反射传播;类似结构还可以参见Datta等人2003年在IEEE SENSORS JOURNAL上第3卷第788-795页发表的文章。或者固体覆盖层利用干涉原理进行光传输,Yin等人在2004年APL 85第3477-3479页上发表的文章中提出了一种由流体导波层和固体覆盖层构成的流体光波导结构,固体覆盖层折射率大于流体折射率,多层覆盖层内的相干干涉使得光在覆盖层发生干涉传播。还可以参见Yin等人在2005年OPTICSEXPRESS上第13期第23号上发表的文章。固体覆盖层组成的流体光波导必须选择合适的材料,或者复杂的制造工艺,使得满足固体覆盖层折射率小于流体的条件。A fluidic optical waveguide composed of a fluidic waveguiding layer and a solid covering layer. A Chinese patent (CN200710044173.3) proposes a fluid optical waveguide structure composed of a fluid waveguide layer and a solid covering layer, and a fluid with a refractive index greater than that of the solid covering layer is selected so that light is fully internal in the fluid waveguiding layer. Reflection propagation; similar structures can also be found in the article published by Datta et al. on pages 788-795 of Volume 3 of IEEE SENSORS JOURNAL in 2003. Or the solid covering layer uses the interference principle to carry out light transmission. In the article published on pages 3477-3479 of APL 85 in 2004, Yin et al. proposed a fluid optical waveguide structure composed of a fluid waveguide layer and a solid covering layer. The solid The refractive index of the covering layer is greater than the refractive index of the fluid, and coherent interference in the multilayer covering layer causes interference propagation of light in the covering layer. See also Yin et al. OPTICS EXPRESS 2005 Issue 13 No. 23. Fluid optical waveguides composed of solid cladding layers must select appropriate materials or complex manufacturing processes to satisfy the condition that the refractive index of the solid cladding layer is lower than that of the fluid.

由流体导波层和气体覆盖层构成的流体光波导。Yang Seung Man等人在欧洲专利(KR20090100956)中提出一种由流体导波层和气体覆盖层构成的光波导。A fluidic optical waveguide composed of a fluidic waveguide layer and a gas cover layer. Yang Seung Man et al. proposed an optical waveguide composed of a fluid waveguide layer and a gas covering layer in European patent (KR20090100956).

由流体导波层和流体覆盖层构成的流体光波导,同样采用折射率大于覆盖层流体折射率的导波层流体,满足光在流体导波层发生全反射传播。Wolfe等人获得的美国专利(US2009/0097808A1)提出了在两种流体处于层流状态时具有小的扩散系数,由折射率数值不同的流体分别形成导波层和覆盖层的流体光波导结构。中国专利(200680005292)提出了一种由两种导电性不同的不相溶流体组成的流体光波导,折射率大的流体作为导波层,该结构能够通过电润湿效应改变液体的分界面以改变光的传输特性。Tang等人在2006年APL 88,061112上发表的文章中描述了一种由不同温度的相同流体组成的流体光波导结构。类似结构还可以参见Li等人在2008年APL 93,193901上发表的文章。由流体覆盖层组成的流体光波导,由于流体之间分子的扩散作用,以及温度场的不稳定性,而影响光在流体光波导中的稳定传播。The fluid optical waveguide composed of the fluid waveguide layer and the fluid cover layer also adopts the waveguide layer fluid whose refractive index is higher than that of the cover layer fluid, so as to satisfy the total reflection propagation of light in the fluid waveguide layer. The US patent (US2009/0097808A1) obtained by Wolfe et al. proposes a fluid optical waveguide structure with a small diffusion coefficient when the two fluids are in a laminar flow state, and a waveguide layer and a cover layer are formed by fluids with different refractive index values. Chinese patent (200680005292) proposes a fluid optical waveguide composed of two immiscible fluids with different conductivity. The fluid with a large refractive index acts as a waveguide layer. This structure can change the interface of the liquid through the electrowetting effect to Change the transmission properties of light. In their article published on APL 88, 061112 in 2006, Tang et al. described a fluidic optical waveguide structure composed of the same fluid at different temperatures. Similar structures can also be found in the article published by Li et al. on APL 93, 193901 in 2008. The fluid optical waveguide composed of a fluid covering layer affects the stable propagation of light in the fluid optical waveguide due to the diffusion of molecules between the fluids and the instability of the temperature field.

发明内容Contents of the invention

本发明的目的是:针对现有由固体覆盖层构成的流体光波导对固体覆盖层和流体导波层材料有限制,以及由流体覆盖层构成的流体光波导因流体之间分子的扩散作用引起的光传播不稳定的现状,提出一种结构简单,能够在流体微管道中实现光稳定传播的流体光波导结构及其应用方法。The purpose of the present invention is: for the existing fluid optical waveguide that is made of solid covering layer, the materials of solid covering layer and fluid waveguide layer are limited, and the fluid optical waveguide made of fluid covering layer is caused by the diffusion of molecules between fluids. Based on the current situation of unstable light propagation, a fluid optical waveguide structure with a simple structure that can realize stable light propagation in a fluid micropipe and its application method are proposed.

参阅附图1和附图2,本发明的技术方案是:一种流体光波导结构,依次包括基底I1、结构层2和基底II3,结构层2上有与基底I1和基底II3平行的微管道,微管道里充满流体,其两端分别与输入口5和输出口7连通,一对金属电极4分别处在基底I1和基底II3上相应的位置上以直接加热微管道中的流体;金属电极4也可以处在结构层2的两个内壁上,或者金属电极4包覆整个微管道;基底I1上在与结构层2上输入口5和输出口7相应的位置上布有开孔,用于流体的输入和输出。Referring to accompanying drawing 1 and accompanying drawing 2, the technical scheme of the present invention is: a kind of fluid light waveguide structure, comprises substrate I1, structural layer 2 and substrate II3 in turn, and the micropipe parallel to substrate I1 and substrate II3 is arranged on structural layer 2 , the micropipe is filled with fluid, and its two ends communicate with the input port 5 and the output port 7 respectively, and a pair of metal electrodes 4 are respectively placed on the corresponding positions on the substrate I1 and the substrate II3 to directly heat the fluid in the micropipe; the metal electrodes 4 can also be located on the two inner walls of the structural layer 2, or the metal electrode 4 covers the whole micropipe; the substrate I1 is provided with openings at positions corresponding to the input port 5 and the output port 7 on the structural layer 2, and the for fluid input and output.

为了保证金属电极4和流体绝缘,在金属电极4表面覆盖聚合物薄膜8,参阅附图7-9。In order to ensure the insulation between the metal electrode 4 and the fluid, the surface of the metal electrode 4 is covered with a polymer film 8, see Figures 7-9.

本发明的有益效果是:基于流体折射率随流体温度的变化而变化的原理形成流体光波导。通过对金属电极4施加恒定电流导致金属电极4温度升高,由于热量传递,微管道中与金属电极4接触的流体区域温度升高,使得该区域流体的折射率降低,在微管道中的流体形成具有不同折射率的区域,与金属电极4接触的区域构成流体覆盖层11,夹在流体覆盖层之间的流体区域构成流体导波层12;由于流体导波层12与流体覆盖层11之间存在折射率梯度,使得光在流体导波层12中稳定传播。The beneficial effect of the present invention is that the fluid optical waveguide is formed based on the principle that the fluid refractive index changes with the fluid temperature. Applying a constant current to the metal electrode 4 causes the temperature of the metal electrode 4 to rise. Due to heat transfer, the temperature of the fluid region in contact with the metal electrode 4 in the micropipe increases, so that the refractive index of the fluid in this region decreases, and the fluid in the micropipe Form regions with different refractive indices, the region in contact with the metal electrode 4 constitutes the fluid covering layer 11, and the fluid region sandwiched between the fluid covering layers constitutes the fluid waveguide layer 12; There is a refractive index gradient between them, so that the light propagates stably in the fluid waveguide layer 12 .

本发明提出的流体光波导结构,采用流体微管道边缘的电极加热方法,使得接触电极区域流体的折射率发生变化,形成流体覆盖层。在微管道中使用任意同种流体制备流体光波导,使得流体光波导的材料选择性更灵活;通过简单的电路控制,实现光在流体光波导中的稳定传播,为生物细胞及生物大分子的光学检测提供了简便工具。The fluid optical waveguide structure proposed by the present invention adopts the electrode heating method at the edge of the fluid micropipe, so that the refractive index of the fluid in the contact electrode area changes to form a fluid covering layer. Using any same fluid in the micropipe to prepare the fluidic optical waveguide makes the material selection of the fluidic optical waveguide more flexible; through simple circuit control, the stable propagation of light in the fluidic optical waveguide can be realized, which is a great support for biological cells and biological macromolecules. Optical inspection provides easy tools.

附图概述Figure overview

图1为一种流体光波导的结构示意图;Fig. 1 is a structural schematic diagram of a fluid optical waveguide;

图2为实施例1中流体光波导6的横截面示意图;FIG. 2 is a schematic cross-sectional view of the fluidic optical waveguide 6 in Embodiment 1;

图3为图2中B-B截面的剖视图;Fig. 3 is the sectional view of B-B section among Fig. 2;

图4为对金属电极4施加恒定电流时流体9的折射率变化与流体9和金属电极4之间距离的关系曲线图;Fig. 4 is a graph showing the relationship between the change in the refractive index of the fluid 9 and the distance between the fluid 9 and the metal electrode 4 when a constant current is applied to the metal electrode 4;

图5A-C为实施例1中流体导波层12和流体覆盖层11之间相对位置关系的示意图;5A-C are schematic diagrams of the relative positional relationship between the fluid waveguide layer 12 and the fluid covering layer 11 in Embodiment 1;

图6为光束10在流体光波导6中传播的示意图;FIG. 6 is a schematic diagram of the beam 10 propagating in the fluidic optical waveguide 6;

图7为实施例2中流体光波导6的横截而示意图;Fig. 7 is a cross-sectional schematic diagram of the fluidic optical waveguide 6 in Embodiment 2;

图8为图7中C-C截面的剖视图;Fig. 8 is the sectional view of C-C section among Fig. 7;

图9为实施例3中流体光波导6的横截面示意图;FIG. 9 is a schematic cross-sectional view of the fluidic optical waveguide 6 in Embodiment 3;

图中:1-基底I,2-结构层,3-基底II,4-金属电极,5-输入口,6-流体光波导,7-输出口,8-聚合物薄膜,9-流体,10-光束,11-流体覆盖层,12-流体导波层。In the figure: 1-substrate I, 2-structural layer, 3-substrate II, 4-metal electrode, 5-input port, 6-fluidic optical waveguide, 7-output port, 8-polymer film, 9-fluid, 10 - light beam, 11 - fluid covering layer, 12 - fluid guiding layer.

具体实施方式Detailed ways

实施例1:Example 1:

参阅附图1和附图2,本发明提出的流体光波导结构依次包括基底I1、结构层2和基底II3,所述基底I1和基底II3材料均为PI,结构层2材料为PDMS;结构层2上有与基底I1和基底II3平行的微管道,微管道里充满去离子水,其两端分别与输入口5和输出口7连通,一对镍金属电极4分别处在基底I1和基底II3上相应的位置上以直接加热微管道中的流体。Referring to accompanying drawings 1 and 2, the fluidic optical waveguide structure proposed by the present invention includes substrate I1, structural layer 2 and substrate II3 in sequence, the materials of substrate I1 and substrate II3 are both PI, and the material of structural layer 2 is PDMS; structural layer There are micro-channels parallel to the substrate I1 and the substrate II3 on the 2. The micro-channels are filled with deionized water, and the two ends of the micro-channels are respectively connected with the input port 5 and the output port 7. A pair of nickel metal electrodes 4 are respectively located on the substrate I1 and the substrate II3. on the corresponding position to directly heat the fluid in the microchannel.

本实施例采用电极加热的方法形成流体光波导。对镍金属电极4施加恒定电流,导致镍金属电极4温度升高,由于热量传递,微管道中与镍金属电极4接触的去离子水区域温度升高,使得该区域去离子水的折射率降低,在微管道中的去离子水形成具有不同折射率的区域,参阅附图4,与镍金属电极4接触的区域构成流体覆盖层11,夹在流体覆盖层11之间的去离子水区域构成流体导波层12,参阅附图5。由于流体导波层12与流体覆盖层11之间存在折射率梯度,使得光束10在流体导波层12中按照附图6的方式传播。In this embodiment, the method of heating electrodes is used to form the fluidic optical waveguide. Applying a constant current to the nickel metal electrode 4 causes the temperature of the nickel metal electrode 4 to rise. Due to heat transfer, the temperature of the deionized water area in contact with the nickel metal electrode 4 in the micropipe increases, so that the refractive index of the deionized water in this area decreases. , the deionized water in the micropipe forms regions with different refractive indices. Referring to accompanying drawing 4, the region in contact with the nickel metal electrode 4 constitutes the fluid covering layer 11, and the deionized water region sandwiched between the fluid covering layers 11 constitutes Fluid waveguide layer 12, refer to accompanying drawing 5. Since there is a refractive index gradient between the fluid waveguide layer 12 and the fluid cover layer 11 , the light beam 10 propagates in the fluid waveguide layer 12 in the manner shown in FIG. 6 .

参阅附图4和附图5,当对基底I1和基底II3上的镍金属电极4施加相同的恒定电流时,基底I1和基底II3上的镍金属电极4温度同步升高,热量的传递速率相同,因此形成高度h相同的流体覆盖层11,流体导波层12处于微管道中间位置;如果施加在基底I1和基底II3上的镍金属电极4的恒定电流不相同,引起两镍金属电极4温度升高的速率不同,导致热量的传递速率不相同,因此形成高度h不相同的流体覆盖层11,流体导波层12偏离微管道中间位置。当施加在基底I1上的镍金属电极4的恒定电流大于施加在基底II3上的镍金属电极4的恒定电流时,流体导波层12向下偏离,如附图5B所示;当施加在基底I1上的镍金属电极4的恒定电流小于施加在基底II3上的镍金属电极4的恒定电流时,流体导波层12向上偏离,如附图5C所示。因此,通过控制施加在基底I1和基底II3上的镍金属电极4的恒定电流大小,改变流体导波层12和流体覆盖层11之间的相对位置关系,实现光束在空间上的调制。Referring to accompanying drawing 4 and accompanying drawing 5, when applying identical constant current to the nickel metal electrode 4 on the substrate I1 and the substrate II3, the temperature of the nickel metal electrode 4 on the substrate I1 and the substrate II3 increases synchronously, and the transfer rate of heat is the same , therefore form the same fluid cover layer 11 with the same height h, and the fluid waveguide layer 12 is in the middle of the micropipe; if the constant current applied to the nickel metal electrode 4 on the substrate I1 and the substrate II3 is not the same, the temperature of the two nickel metal electrodes 4 will be caused The different rising rates lead to different heat transfer rates, thus forming fluid covering layers 11 with different height h, and the fluid waveguide layer 12 deviates from the middle position of the micropipe. When the constant current applied to the nickel metal electrode 4 on the substrate I1 is greater than the constant current applied to the nickel metal electrode 4 on the substrate II3, the fluid waveguide layer 12 deviates downward, as shown in Figure 5B; when applied to the substrate When the constant current of the nickel metal electrode 4 on I1 is smaller than the constant current of the nickel metal electrode 4 applied on the substrate II3, the fluid waveguide layer 12 deviates upward, as shown in FIG. 5C . Therefore, by controlling the magnitude of the constant current applied to the nickel metal electrodes 4 on the substrates I1 and II3, the relative positional relationship between the fluid waveguide layer 12 and the fluid covering layer 11 is changed to achieve spatial modulation of the beam.

由于一对镍金属电极4分别处在基底I1和基底II3上相应的位置上,当对镍金属电极4施加恒定电流时,引起微管道中与其接触的去离子水的折射率发生变化,仅在垂直于基底I1和基底II3方向上满足流体导波层12的折射率大于流体覆盖层11的折射率,因此形成平面波导。Since a pair of nickel metal electrodes 4 are respectively located at the corresponding positions on the substrate I1 and the substrate II3, when a constant current is applied to the nickel metal electrodes 4, the refractive index of the deionized water in contact with the micropipelines changes, only at In the direction perpendicular to the substrate I1 and the substrate II3, the refractive index of the fluid waveguide layer 12 is greater than the refractive index of the fluid covering layer 11, thus forming a planar waveguide.

实施例2:Example 2:

参阅附图7和附图8,本发明提出的流体光波导结构依次包括基底I1、结构层2和基底II3,所述基底I1和基底II3材料均为PMMA,结构层2材料为PDMS;结构层2上有与基底I1和基底II3平行的微管道,微管道里充满乙醇,其两端分别与输入口5和输出口7连通,一对铜金属电极4分别处在结构层2的两个内壁上以直接加热微管道中的流体。为了保证金属电极4和乙醇绝缘,在金属电极4表面覆盖材料为聚乙烯醇的聚合物薄膜8。Referring to accompanying drawing 7 and accompanying drawing 8, the fluid optical waveguide structure that the present invention proposes comprises substrate I1, structural layer 2 and substrate II3 successively, and described substrate I1 and substrate II3 material are all PMMA, and structural layer 2 material is PDMS; There are micro-pipes parallel to the base I1 and base II3 on the 2, the micro-pipes are filled with ethanol, and the two ends of the micro-pipes are respectively connected with the input port 5 and the output port 7, and a pair of copper metal electrodes 4 are respectively located on the two inner walls of the structural layer 2 above to directly heat the fluid in the microchannel. In order to ensure the insulation between the metal electrode 4 and ethanol, the surface of the metal electrode 4 is covered with a polymer film 8 made of polyvinyl alcohol.

本实施例采用电极加热的方法形成流体光波导。对铜金属电极4施加恒定电流,导致铜金属电极4温度升高,出于热量传递,微管道中与铜金属电极4接触的乙醇区域温度升高,使得该区域乙醇的折射率降低,在微管道中的乙醇形成具有不同折射率的区域,与铜金属电极4接触的区域构成流体覆盖层11,夹在流体覆盖层11之间的乙醇区域构成流体导波层12。In this embodiment, the method of heating electrodes is used to form the fluidic optical waveguide. Applying a constant current to the copper metal electrode 4 causes the temperature of the copper metal electrode 4 to rise. Due to heat transfer, the temperature of the ethanol region in contact with the copper metal electrode 4 in the micropipe increases, so that the refractive index of the ethanol in this region decreases. The ethanol in the pipeline forms regions with different refractive indices, the region in contact with the copper metal electrode 4 constitutes the fluid covering layer 11 , and the ethanol region sandwiched between the fluid covering layers 11 constitutes the fluid waveguide layer 12 .

由于铜金属电极4处在结构层2的两个内壁上,当对铜金属电极4施加恒定电流时,引起微管道中与其接触的乙醇的折射率发生变化,仅在垂直于内壁方向上满足流体导波层12的折射率大于流体覆盖层11的折射率,因此形成平面波导。Since the copper metal electrodes 4 are located on the two inner walls of the structural layer 2, when a constant current is applied to the copper metal electrodes 4, the refractive index of the ethanol in contact with the copper metal electrodes in the micropipes changes, and only in the direction perpendicular to the inner walls can the fluid The waveguide layer 12 has a higher refractive index than the fluid cover layer 11, thus forming a planar waveguide.

实施例3:Example 3:

参阅附图9,本发明提出的流体光波导结构依次包括基底I1、结构层2和基底II3,所述基底I1和基底II3材料均为玻璃,结构层2材料为SU-8;结构层2上有与基底I1和基底II3平行的微管道,微管道里充满氯化钙溶液,其两端分别与输入口5和输出口7连通,镍铝合金电极4包覆整个微管道以直接加热微管道中的流体。为了保证镍铝合金金属电极4和氯化钙溶液绝缘,在镍铝合金金属电极4表面覆盖材料为PI的聚合物薄膜8。因制作工艺误差的存在,导致基底I1和基底II3上的镍铝合金金属电极与结构层2内壁上的镍铝合金金属电极不能够完好地接触,因此,在基底I1和基底II3上制作镍铝合金金属电极时,使镍铝合金金属电极的宽度大于微管道的宽度。Referring to accompanying drawing 9, the fluidic optical waveguide structure proposed by the present invention includes substrate I1, structural layer 2 and substrate II3 in sequence, the materials of substrate I1 and substrate II3 are both glass, and the material of structural layer 2 is SU-8; There are micro-channels parallel to the substrates I1 and II3. The micro-channels are filled with calcium chloride solution, and their two ends are respectively connected to the input port 5 and the output port 7. The nickel-aluminum alloy electrode 4 covers the entire micro-channel to directly heat the micro-channel. fluid in. In order to ensure the insulation between the nickel-aluminum alloy metal electrode 4 and the calcium chloride solution, the surface of the nickel-aluminum alloy metal electrode 4 is covered with a polymer film 8 made of PI. Due to the existence of manufacturing process errors, the nickel-aluminum alloy metal electrodes on the substrate I1 and the substrate II3 cannot be in good contact with the nickel-aluminum alloy metal electrodes on the inner wall of the structure layer 2. Therefore, the nickel-aluminum alloy metal electrodes on the substrate I1 and the substrate II3 are fabricated When using an alloy metal electrode, the width of the nickel-aluminum alloy metal electrode is greater than the width of the micropipe.

本实施例采用电极加热的方法形成流体光波导。对镍铝金属电极4施加恒定电流,导致镍铝金属电极4温度升高,由于热量传递,微管道中与镍铝金属电极4接触的氯化钙溶液区域温度升高,使得该区域氯化钙溶液的折射率降低,在微管道中的氯化钙溶液形成具有不同折射率的区域,与镍铝金属电极4接触的区域构成流体覆盖层11,夹在流体覆盖层11之间的氯化钙溶液区域构成流体导波层12。In this embodiment, the method of heating electrodes is used to form the fluidic optical waveguide. Applying a constant current to the nickel-aluminum metal electrode 4 causes the temperature of the nickel-aluminum metal electrode 4 to rise. Due to heat transfer, the temperature of the calcium chloride solution area in contact with the nickel-aluminum metal electrode 4 in the micropipe increases, so that the calcium chloride in this area The refractive index of solution reduces, and the calcium chloride solution in micropipe forms the zone with different refractive index, and the zone that contacts with nickel-aluminum metal electrode 4 constitutes fluid covering layer 11, and the calcium chloride that is sandwiched between fluid covering layer 11 The solution region constitutes the fluidic waveguiding layer 12 .

由于镍铝合金金属电极4包覆整个微管道,当对镍铝合金金属电极4施加恒定电流时,引起微管道中与其接触的氯化钙溶液的折射率发生变化,在任意方向上均满足流体导波层12的折射率大于流体覆盖层11的折射率,光束能够在流体导波层12中沿任意方向传播,因此形成柱形波导。Since the nickel-aluminum-aluminum metal electrode 4 covers the entire micropipe, when a constant current is applied to the nickel-aluminum-aluminum metal electrode 4, the refractive index of the calcium chloride solution in the micropipe in contact with it changes, and the flow rate of the fluid in any direction is satisfied. The refractive index of the wave guiding layer 12 is greater than that of the fluid covering layer 11 , and light beams can propagate in any direction in the fluid guiding layer 12 , thus forming a cylindrical waveguide.

Claims (4)

1.一种流体光波导结构,依次包括基底I(1)、结构层(2)和基底II(3),结构层(2)上有与基底I(1)和基底II(3)平行的微管道,微管道里充满流体,其两端分别与输入口(5)和输出口(7)连通,一对金属电极(4)分别处在基底I(1)和基底II(3)上相应的位置上以直接加热微管道中的流体;基底I(1)上与结构层(2)上输入口(5)和输出口(7)相应的位置上布有开孔,用于流体的输入和输出。1. A fluid optical waveguide structure, comprising a substrate I (1), a structural layer (2) and a substrate II (3) in turn, the structural layer (2) has a substrate parallel to the substrate I (1) and the substrate II (3) The micro-pipe is filled with fluid, and the two ends of the micro-pipe are respectively connected with the input port (5) and the output port (7). A pair of metal electrodes (4) are located on the substrate I (1) and the substrate II (3) respectively. on the position to directly heat the fluid in the micropipe; on the substrate I (1) and the corresponding positions of the input port (5) and the output port (7) on the structural layer (2), holes are arranged for the input of the fluid and output. 2.一种如权利要求1所述的流体光波导结构,其特征在于:所述的金属电极(4)位置替换为处在结构层(2)的两个内壁上。2. A fluidic optical waveguide structure according to claim 1, characterized in that: the position of the metal electrode (4) is replaced by being located on the two inner walls of the structural layer (2). 3.一种如权利要求1所述的流体光波导结构,其特征在于:所述的金属电极(4)位置替换为包覆整个微管道。3. A fluidic optical waveguide structure according to claim 1, characterized in that: the position of the metal electrode (4) is replaced by covering the entire micropipe. 4.一种如权利要求1-3所述之一的流体光波导结构,其特征在于:所述的在金属电极表面覆盖聚合物薄膜(8)。4. A fluidic optical waveguide structure according to any one of claims 1-3, characterized in that the surface of the metal electrode is covered with a polymer film (8).
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