CN115290616A - Polymer Optical Waveguide Evanescent Field Sensing Structure - Google Patents
Polymer Optical Waveguide Evanescent Field Sensing Structure Download PDFInfo
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Abstract
Description
技术领域technical field
本发明涉及一种平面波导传感结构,具体是关于一种激发大范围消逝场照明区域的传感结构,应用领域包括生物检测、显微成像。The invention relates to a planar waveguide sensing structure, in particular to a sensing structure that excites a large-scale evanescent field illumination area, and its application fields include biological detection and microscopic imaging.
背景技术Background technique
自上世纪60年代初,生物传感器被首次提出并验证了可行性,该领域就随着生化技术和微电子等技术的进步不断发展壮大。在诸多生物传感技术中,荧光生物传感器以其灵敏度高、选择性好、实时性强等诸多优点被广泛应用,但由于散射光、生物样品自荧光和无效发射荧光等的干扰,使得此类传感器往往需要使用复杂的光学系统来提高信噪比,为此,消逝场照明被应用于荧光生物传感领域。Since the early 1960s, biosensors were first proposed and verified to be feasible, and this field has continued to grow and develop with the advancement of technologies such as biochemical technology and microelectronics. Among many biosensing technologies, fluorescent biosensors are widely used due to their high sensitivity, good selectivity, and strong real-time performance. Sensors often need to use complex optical systems to improve the signal-to-noise ratio. For this reason, evanescent field illumination is used in the field of fluorescent biosensing.
当光从光密介质入射到光疏介质时,折射光会随着入射角的增加逐渐偏离法线,直到光线沿着两介质的分界面传播,此时折射角为90度,随着入射光的入射角继续增加,光疏介质中不再出现折射光,入射光会被完全反射回光密介质中,将刚开始发生全反射的入射角称为临界角,并将这种现象称为光的全内反射。电磁场的边界连续性条件表明,介质分界面发生全发射时,在光密介质表面会产生一个极速衰减、高度受限的非均匀场,该场即为消逝场。消逝场具有和入射光相同的波长,且强度随远离波导表面的距离呈指数衰减,对于可见波段(380-780纳米)入射光而言,只会在波导表层形成百纳米的消逝场照明区域。消逝场的穿透深度被定义为能量衰减到初始能量1/e处的位置,通过改变入射光波长、入射角度或者材料相对折射率等因素可以改变消逝场的穿透深度。When light is incident from an optically denser medium to an optically rarer medium, the refracted light will gradually deviate from the normal line as the incident angle increases until the light propagates along the interface between the two media. At this time, the refraction angle is 90 degrees. The incident angle continues to increase, the refracted light will no longer appear in the optically sparse medium, and the incident light will be completely reflected back into the optically dense medium. The incident angle at which total reflection begins to occur is called the critical angle, and this phenomenon is called light of total internal reflection. The boundary continuity condition of the electromagnetic field shows that when full emission occurs at the interface of the medium, a non-uniform field with extremely fast attenuation and height limitation will be generated on the surface of the optically dense medium, which is the evanescent field. The evanescent field has the same wavelength as the incident light, and its intensity decays exponentially with the distance away from the waveguide surface. For the incident light in the visible band (380-780 nanometers), only a hundred nanometers of evanescent field illumination area will be formed on the surface of the waveguide. The penetration depth of the evanescent field is defined as the position where the energy decays to the
用于生物检测的荧光标记物的激发波长大多数位于可见光波段,在该波段激发的消逝场深度远小于细胞的平均直径,这意味着只有靠近波导表面的荧光标记物能够被激发,这种照明激发方式在仅选择性的激发目标荧光的同时,极大降低了入射光、散射光、细胞自发荧光以及背景荧光的干扰,使得检测系统的信噪比得到极大提高。Most of the excitation wavelengths of fluorescent markers used for biological detection are in the visible light band, and the depth of the evanescent field excited in this band is much smaller than the average diameter of cells, which means that only fluorescent markers close to the surface of the waveguide can be excited. The excitation method only selectively excites the target fluorescence, while greatly reducing the interference of incident light, scattered light, cell autofluorescence and background fluorescence, so that the signal-to-noise ratio of the detection system is greatly improved.
基于消逝场荧光原理的生物传感器件已经被应用于细胞成像、环境监测、药物开发和体外诊断等诸多领域,为了使得此类传感器获得更高的信噪比、检测范围、均一性和集成度,并实现多波长检测,降低生产使用成本,传感器的结构、材料、配套系统和荧光标记方法等一直在得到改进。结构上,消逝场传感照明的典型结构包括光纤和平面波导两种,光纤型结构具有体积小、灵敏度高、抗干扰能力强等优势,但其能够提供的检测区域较小、操作和制造要求较为复杂。因此,在实际应用中平面波导由于传感面积大、耦合方式多样、制造相对简单等诸多优点被优先选择。此外,常见的平面波导耦合方式包括直接耦合、棱镜耦合、透镜耦合、光栅耦合等,其中透镜耦合在对入射光进行偏折的同时具有汇聚效果,相比之下,使用该方法进行入射光耦合,不需要配套复杂的对准和调角装置,同时,聚焦效果使得入射光在波导内发生一定距离连续全内反射后,将在波导表面产生连续成看的大范围照明传感区域。在材料上,早期的消逝场传感结构是基于玻璃载玻片研发的,然而,玻璃材料在进行不规则结构加工时存在极大限制,因此,高透聚合物材料的传感特性成为该领域的研究重点,以在保证传感性能的同时降低制造难度和生产成本,使得此类传感器的规模化使用成为可能。Biosensor devices based on the principle of evanescent field fluorescence have been applied in many fields such as cell imaging, environmental monitoring, drug development and in vitro diagnosis. In order to make such sensors obtain higher signal-to-noise ratio, detection range, uniformity and integration, And to achieve multi-wavelength detection, reduce the cost of production and use, the structure, material, supporting system and fluorescent labeling method of the sensor have been improved. Structurally, the typical structure of evanescent field sensing lighting includes optical fiber and planar waveguide. The optical fiber structure has the advantages of small size, high sensitivity, and strong anti-interference ability, but the detection area it can provide is small, and the operation and manufacturing requirements more complicated. Therefore, in practical applications, planar waveguides are preferred due to many advantages such as large sensing area, various coupling methods, and relatively simple manufacturing. In addition, common planar waveguide coupling methods include direct coupling, prism coupling, lens coupling, grating coupling, etc., where the lens coupling has a converging effect while deflecting the incident light. In contrast, using this method for incident light coupling , without the need for supporting complex alignment and angle adjustment devices. At the same time, the focusing effect makes the incident light undergo continuous total internal reflection at a certain distance in the waveguide, and a continuous large-scale illumination sensing area will be produced on the surface of the waveguide. In terms of materials, the early evanescent field sensing structure was developed based on glass slides. However, glass materials have great limitations in the processing of irregular structures. The research focus is to reduce the manufacturing difficulty and production cost while ensuring the sensing performance, making the large-scale use of such sensors possible.
目前,尚未有一种可量产化的消逝场传感结构/系统,在实现高传感区域均一性、高集成度的同时,实现大有效传感区域、快速多波长检测,为此,为了进一步提高消逝场荧光传感器的性能、降低生产使用成本、实现多场景应用,开发一种基于聚合物集成平板波导的传感结构/系统十分必要。At present, there is no evanescent field sensing structure/system that can be mass-produced, which can achieve large effective sensing area and fast multi-wavelength detection while achieving high sensing area uniformity and high integration. Therefore, in order to further To improve the performance of evanescent field fluorescence sensors, reduce production and use costs, and realize multi-scenario applications, it is necessary to develop a sensing structure/system based on polymer-integrated slab waveguides.
发明内容Contents of the invention
本发明公开了一种在可见光波段具有波长鲁棒性的改进型消逝场照明传感结构,该结构通过耦合结构将输入光耦合到薄层平面波导内,从而实现入射光在波导内发生连续全内反射,具体结构如图1所示,包括耦合结构110、薄层波导结构120和裙边结构130,各结构的特征在于:The invention discloses an improved evanescent field illumination sensing structure with wavelength robustness in the visible light band. The structure couples the input light into the thin-layer planar waveguide through the coupling structure, so as to realize the continuous and full generation of the incident light in the waveguide. Internal reflection, the specific structure is shown in Figure 1, including a
耦合结构110位于照明传感结构的前端,由透镜111和多边形棱镜112集成而来。所述透镜111的面型设计为非球面,从而消除由透镜结构带来的球差,并最小化了380-780nm可见光波段内的色差,该结构至少包含一个完整柱面的四分之一;所述多边形棱镜112的短边位置应不超过输入光在薄层波导内的第二反射点位置,从而避免耦合结构与薄层波导之间的失配,导致入射光直接从耦合结构穿过,该结构还设置有一切角斜面,可以起到安装限位的作用。The
薄层波导结构120位于照明传感结构的后端,该结构的长宽为标准载玻片尺寸,如75mm×25mm,波导的厚度介于0.05-0.8mm。The thin-
裙边结构130被设置在薄层波导结构的下表面,与薄层波导为一体化结构,该结构可以减小薄层波导由于加工应力引起的Z向翘曲,该值应小于0.5mm;该结构还起到垫片的效果,以在波导表面与上层结构之间形成流体腔。裙边结构设置在薄层结构的上表面,也可以达到类似的效果。The
本发明采用高精密模具对波导结构进行注塑成型,将耦合结构110、薄层波导结构120和裙边结构130 一体化集成,其中,针对耦合结构110的透镜111和多边形棱镜112进行了镶件模具设计,如图2(c)所 示,以便后续对结构做进一步优化改进。此外,对于厚度低于0.4mm的聚合物薄层波导,可以采用拼接方 式进行加工,耦合结构110采用镶件模具进行成型加工,如图2(d)所示,薄层波导结构120和裙边结构 130采用另一模具一体化注塑成型,采用折射率匹配液实现两加工后结构的粘合拼接。The present invention uses a high-precision mold to perform injection molding on the waveguide structure, and integrates the
本发明涉及的消逝场照明传感结构满足以下特点:耦合结构110、薄层波导结构120和裙边结构130 均采用相同的材料进行加工,材料的折射率介于1.44-2.50之间,且对于波长为380-780nm的入射光透明,材料根据采用加工方法不同,可选用光学聚合物或光学玻璃。如图3所示的结构中,波导结构的上表面310、下表面320以及耦合结构的自由曲面330的粗糙度小于10nm,波导结构的上平面310的平整度小于0.5mm,波导结构的Z向翘曲度小于0.5mm,波导结构的厚度公差被控制在±0.05mm以内,照明传感结构的侧面340 的表面粗糙度小于100nm;为提高入射光的利用效率,可对自由曲面330进行镀膜增透处理。The evanescent field illumination sensing structure involved in the present invention satisfies the following characteristics: the
本发明还公开了一种用于产生大范围均匀消逝场照明区域光学系统。输入激光经过准直后,入射到光束整形元件上,之后以一定角度发射出能量分布均匀的光斑,经过柱状透镜后可得到不发散的准直整形光斑,准直光斑水平入射到传感结构的耦合结构,将以大于全内反射临界角的入射角聚焦到薄层波导结构的上表面,光束在薄层波导结构内发生连续的全内反射后,最终在薄层波导表面的消逝场初始能量趋于稳定,形成大范围、均一性高的传感检测区域。该系统具体如图4所示,包括光源部分410、照明传感结构420、检测区域430。各部分的主要特征如下:The invention also discloses an optical system for producing large-scale uniform evanescent field illumination area. After the input laser is collimated, it is incident on the beam shaping element, and then emits a light spot with uniform energy distribution at a certain angle. After passing through the cylindrical lens, a collimated and shaped light spot that does not diverge can be obtained. The collimated light spot is horizontally incident on the sensor structure. The coupling structure focuses the incident angle greater than the critical angle of total internal reflection onto the upper surface of the thin-layer waveguide structure. After the beam undergoes continuous total internal reflection in the thin-layer waveguide structure, the initial energy of the evanescent field on the surface of the thin-layer waveguide is finally tends to be stable, forming a large-scale, high-uniformity sensing area. The system is specifically shown in FIG. 4 , including a
所述的光源部分410由光源411、准直透镜412、整形器件413和柱状透镜414组成。光源采用激光器二极管(LD)或者发光二极管(LED);根据光源发散角和所需光斑大小,准直透镜将来自光源的发散光斑准直成沿水平方向传播的光束;整形器件将准直圆光斑变成线状、椭圆、矩形或正方形的光斑,同时改善光斑能量分布,本发明采用衍射光学元件(DOE)、鲍威尔透镜(Powell Lens)、微透镜阵列(MLA)或柱状透镜对光斑实现整形。The
所述照明传感结构420,其前端的耦合结构将整形后的入射光耦合进薄层波导结构内进行传输,入射光在薄层波导内传输的同时能量发生衰减,其表面能量在接近薄层波导末端时趋于稳定;由于前端耦合透镜的汇聚作用,使得光束由连续平行式全内反射,变成多模式的连续全内反射,不同模式间的混合,最终在波导末端形成连续成片的均匀照明区域,光路示意如图5所示。The
所述检测区域430,区域被设置在照明传感结构420的末端,该区域的尺寸被设置为不低于10mm× 10mm,且区域内的照明均一性要求低于10%,该区域还设有一定数量的样品固定点,被荧光物质标记的待检测物质由这些点固定在薄层波导表面,经过消逝场激发后即可实现荧光生物传感。The
本发明还提供了一种利用大范围均匀消逝场照明区域进行荧光分析的生物检测系统,系统的主要结构如图6所示,系统围绕着照明传感波导630搭建,还包括:光源部分610、位移结构620、承载结构640、滤光系统650和成像系统660。光源发射出的光束经过整形后,被耦合结构以大于全内反射临界角的入射角耦合进薄层波导内,光束在薄层波导内发生连续全内反射后在波导末端形成连片的高均一性消逝场照明区域,位于波导表面的荧光标记待检测物质经消逝场激发后,发射出特定波长的荧光信号,光信号经过滤光系统后将只通过特定波段的荧光信号,荧光信号经过成像系统的捕获后,最终经过图像处理后得到传感结果。系统各部分特征如下:The present invention also provides a biological detection system for fluorescence analysis using a large-scale uniform evanescent field illumination area. The main structure of the system is shown in FIG.
光源部分610用于提供沿水平方向传播的光束,并完成对光束的准直、整形等,使输出的光束为能量分布均匀的整形光斑。The
位移结构620可以实现光源相对于传感波导在水平和垂直两个自由度上的位移,用于调节光源与传感波导之间的相对位置,其中水平方向的位移可以改变输入光入射到耦合结构上的水平位置,以实现水平方向上的图像拼接,垂直方向的位移可以改变输入光入射到耦合结构上的垂直位置,以实现入射光以不同入射角度耦合进入薄层波导结构。在一实施例中,该结构能够分别在水平和垂直方向实现25mm的位移。The
照明传感波导630通过前端耦合结构将入射光耦合到薄层波导结构内传输,进而在薄层波导的表面产生消逝场照明区域;在薄层波导表面末端设置有一定数量的待测样品固定点,固定点根据待测样品的种类、固定方式不同,采用不同的斑点大小和排列方式,固定点可以预制在波导表面,也可以根据需求在不同应用场景下进行现场制作。The
承载结构640通过夹持结构来支撑并固定照明传感波导630。The carrying
滤光系统650根据输入光波长和发射荧光波长配有不同滤光片,为提高系统滤光效果可选用多个滤光片形成滤光片组,从而对来自检测区域的光进行过滤,使得仅荧光物质发射的荧光能够通过;滤光片/组被安装在一个镜筒中,并进一步安装到成像系统。The
成像系统660通过sCMOS或CCD相机对荧光信号进行捕获,为简化系统可以采用sCMOS或CCD芯片进行替换;成像相机或芯片将采集到的荧光图像传送到计算机,并对图像进行处理分析,进而得到传感结果。The
附图说明Description of drawings
图1是本发明聚合物消逝场光波导传感结构示意图Fig. 1 is a schematic diagram of the polymer evanescent field optical waveguide sensing structure of the present invention
图2是本发明光波导传感结构加工方案示意图Fig. 2 is a schematic diagram of the processing scheme of the optical waveguide sensing structure of the present invention
图3是本发明光波导传感结构各面标注说明示意图Figure 3 is a schematic diagram illustrating the labeling of each surface of the optical waveguide sensing structure of the present invention
图4是本发明用于产生大范围均匀消逝场照明区域光学系统示意图Fig. 4 is a schematic diagram of the optical system for producing a large-scale uniform evanescent field illumination area according to the present invention
图5是本发明光波导传感结构和此前棱镜耦合传感结构光路示意图Fig. 5 is a schematic diagram of the optical path of the optical waveguide sensing structure of the present invention and the previous prism coupling sensing structure
图6是本发明荧光分析生物检测流程图与系统图Fig. 6 is the flow chart and system diagram of fluorescence analysis biological detection of the present invention
图7是本发明光波导传感结构实际加工样品测试参数结果图Fig. 7 is a graph showing the test parameter results of the actual processing sample of the optical waveguide sensing structure of the present invention
图8是本发明光波导传感结构光学耦合测试实物与结果图Fig. 8 is the real object and result diagram of the optical coupling test of the optical waveguide sensing structure of the present invention
图9是本发明光波导传感结构在COC材料条件下,上表面局部能量分布曲线图Fig. 9 is a curve diagram of local energy distribution on the upper surface of the optical waveguide sensing structure of the present invention under the condition of COC material
图10本发明光波导传感结构多波长检测区域结果示意图Figure 10 is a schematic diagram of the results of multi-wavelength detection regions of the optical waveguide sensing structure of the present invention
具体实施方式Detailed ways
为进一步说明本发明的技术要点,以下将结合附图和实例对本发明做详细说明。In order to further illustrate the technical points of the present invention, the present invention will be described in detail below in conjunction with the accompanying drawings and examples.
如图1所示的照明传感结构,本发明给出了一个实施例,其中耦合结构110的透镜111的面型采用二阶非球面,其中圆锥常数k为-0.56、曲率半径c为0.3,则面型方程为:The illumination sensing structure shown in Figure 1, the present invention provides an embodiment, wherein the surface type of the
波导结构120的长宽为75mm×25mm,其厚度采用0.8mm和0.6mm两种尺寸,波导下端设置有1mm宽的裙边结构333,The length and width of the
照明传感结构加工采用高精密模具进行注塑成型,分别采用聚苯乙烯(PS)、聚碳酸甲酯(PC)、环烯烃共聚物(COC)、聚甲基丙烯酸甲酯(PMMA)四种材料进行一体化注塑加工,针对实施例加工得到的照明传感结构还需进行抛光处理。使用粗糙度测量仪对结构的粗糙度进行测量,使用高度规和CNC投影仪对波导结构的平整度、翘曲度和长宽公差进行了测试,结果如图7所示,显然各项参数均满足设计需求,且裙边结构130的引入有效控制了波导结构的Z向翘曲度。The processing of the lighting sensor structure adopts high-precision molds for injection molding, and four materials are used: polystyrene (PS), polymethyl carbonate (PC), cycloolefin copolymer (COC), and polymethyl methacrylate (PMMA). For integrated injection molding processing, the lighting sensing structure processed in the embodiment needs to be polished. The roughness of the structure was measured with a roughness measuring instrument, and the flatness, warpage, and length and width tolerances of the waveguide structure were tested with a height gauge and a CNC projector. The results are shown in Figure 7. Obviously, all parameters are consistent. The design requirements are met, and the introduction of the
在另一实施例中,输入光源为波长为520nm的激光二极管,激光经过一准直透镜后的到直径1mm的圆形准直光斑,光斑经过通过直径为1mm的光阑后输出光功率为5.24mW,准直光束沿水平方向入射到照明传感结构的耦合结构,照明传感结构采用PS材料制成,在520nm处的折射率为1.60,上层介质为空气,则发生全内反射临界角为38.68°,In another embodiment, the input light source is a laser diode with a wavelength of 520nm, and the laser beam passes through a collimating lens to a circular collimated spot with a diameter of 1mm, and the output light power of the spot after passing through a diaphragm with a diameter of 1mm is 5.24 mW, the collimated light beam is incident on the coupling structure of the illumination sensing structure along the horizontal direction, the illumination sensing structure is made of PS material, the refractive index at 520nm is 1.60, and the upper medium is air, then the critical angle of total internal reflection is 38.68°,
经过耦合结构的偏折与聚焦,光束被很好的耦合到传感波导结构内进行传输,测量波导结构上表面的能量分布如图8所示,结果由五次测量平均而来,曲线前端的平坦部分是验证系统处于稳定状态,此后为波导上表面沿光传输方向的光功率分布,开始表现为能量衰减,随着光束在波导内传输能量分布趋于稳定,在接近波导结构末端形成较为均匀平坦的照明区域。After the deflection and focusing of the coupling structure, the light beam is well coupled into the sensing waveguide structure for transmission. The energy distribution on the upper surface of the measured waveguide structure is shown in Figure 8. The results are averaged from five measurements. The front end of the curve is The flat part is to verify that the system is in a stable state. After that, it is the optical power distribution along the optical transmission direction on the upper surface of the waveguide, which begins to show energy attenuation. As the light beam transmits in the waveguide, the energy distribution tends to be stable, and a more uniform shape is formed near the end of the waveguide structure. Flat lighting area.
基于传感照明结构100,本发明进一步提供了一种用于产生大范围均匀消逝场照明区域光学系统,示意图如图4所示。系统工作时,由光源411发射出的圆斑发散光束经过准直透镜412后,得到一束平行出射的圆斑准直光束,此时光斑能量成高斯型分布,经由整形器件413后,准直圆斑被转变成一束扁椭圆/ 正方形/矩形/线形发散光斑,此时的光斑能量分布均匀,由柱状透镜414对整形后光斑再次进行准直,可得到一束能量分布均匀的扁椭圆/正方形/矩形/线形准直光斑,准直整形光斑由照明传感结构420前端的耦合结构耦合并聚焦到波导结构的上表面,并在此介质分界面处发生全内反射,此后准直整形光斑在波导内发生连续的全内反射,随着在波导内传输的距离增加,在波导上下表面会形成连续成片的均匀消逝场照明区域,本发明采用变异系数CV(Coefficient of Variation)来衡量此区域的能量分布均一性:Based on the
其中σ为区域内能量的平均值,μ表示能量分布的标准差,本发明采用CV<10%的消逝场照明区域选作为检测区域430,该区域可预制/现场制作一定数量的样品捕获点用于固定生物样品,带荧光标记物的生物样品在高均一性的消逝场照明激发下,将发射特定波长的荧光信号。Wherein σ is the average value of the energy in the area, and μ represents the standard deviation of the energy distribution. The present invention adopts the evanescent field illumination area with CV<10% as the
图9显示的是COC材料的照明传感结构上表面局部能量分布曲线,波导结构厚度为0.8mm,结果表明,波导结构上表面的能量随着光的传输距离增加而趋于稳定,最终在波导结构的末端形成均一性低于10%的照明区域,该区域即在本发明中被设定的检测区域430。Figure 9 shows the local energy distribution curve on the upper surface of the illumination sensing structure of the COC material. The thickness of the waveguide structure is 0.8 mm. The end of the structure forms an illumination area with a uniformity lower than 10%, which is the
图10显示的是采用本发明提出消逝场照明光学系统400在三种不同波长输入光条件下,COC材料照明传感结构上表面能够形成的多波长检测区域的大小。三种波长为常用荧光激发光波长,分别为488nm、520nm 和646nm,入射光通过前端的耦合结构110进行耦合,由于色差的存在,在波导结构120的上表面会形成不同的消逝场照明场分布,计算三种波长激发的CV<10%的照明场的重合区域,该区域具有波长鲁棒性,能够被用于样品多色检测。FIG. 10 shows the size of the multi-wavelength detection area that can be formed on the upper surface of the sensor structure illuminated by the COC material under the condition of input light of three different wavelengths using the evanescent field illumination optical system 400 proposed by the present invention. The three wavelengths are commonly used fluorescence excitation wavelengths, respectively 488nm, 520nm and 646nm. The incident light is coupled through the
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CN103063640A (en) * | 2012-12-28 | 2013-04-24 | 西北核技术研究所 | Laser-induced fluorescence combustion field parameter measuring device |
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