CN111912524B - Raman spectroscopy imaging method and imaging device - Google Patents

Raman spectroscopy imaging method and imaging device Download PDF

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CN111912524B
CN111912524B CN201911356312.5A CN201911356312A CN111912524B CN 111912524 B CN111912524 B CN 111912524B CN 201911356312 A CN201911356312 A CN 201911356312A CN 111912524 B CN111912524 B CN 111912524B
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CN111912524A (en
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王斌
徐晓轩
梁菁
王浩
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Nankai University
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
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    • G01J3/2823Imaging spectrometer
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
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    • G01J3/0205Optical elements not provided otherwise, e.g. optical manifolds, diffusers, windows
    • G01J3/0208Optical elements not provided otherwise, e.g. optical manifolds, diffusers, windows using focussing or collimating elements, e.g. lenses or mirrors; performing aberration correction
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    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
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    • G01J3/44Raman spectrometry; Scattering spectrometry ; Fluorescence spectrometry
    • G01J3/4412Scattering spectrometry
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    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/63Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
    • G01N21/65Raman scattering
    • G01N21/658Raman scattering enhancement Raman, e.g. surface plasmons
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B13/00Optical objectives specially designed for the purposes specified below
    • G02B13/001Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras
    • G02B13/0015Miniaturised objectives for electronic devices, e.g. portable telephones, webcams, PDAs, small digital cameras characterised by the lens design

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Abstract

The invention relates to a Raman spectrum imaging device, which belongs to the technical field of spectrum imaging, wherein in the prior art, corresponding objective lenses are not specially designed for different substrates; the method has wide application, can be selected according to the characteristics of the detection object, and can also be used for comparison and scientific research.

Description

一种拉曼光谱成像方法和成像装置Raman spectroscopy imaging method and imaging device

技术领域technical field

本发明涉及光谱成像技术领域,具体涉及一种拉曼光谱成像装置。The invention relates to the technical field of spectral imaging, in particular to a Raman spectral imaging device.

背景技术Background technique

拉曼光谱是一种散射光谱,是印度科学家C.V.拉曼所发现的。基于拉曼散射效应,对与入射光频率不同的散射光谱进行分析以得到分子振动、转动方面的信息,并应用于分子结构研究具有很大的价值。Raman spectroscopy is a type of scattering spectroscopy discovered by Indian scientist C.V. Raman. Based on the Raman scattering effect, it is of great value to analyze the scattering spectrum with different frequencies from the incident light to obtain information on molecular vibration and rotation, and to apply it to the study of molecular structure.

但是拉曼散射效应是个非常弱的过程,所以拉曼信号都很弱,要对表面吸附物种进行拉曼光谱研究几乎都要利用某种增强效应。现有技术中,最常见的表面增强拉曼光谱效应,表面增强拉曼光谱的基底是关键技术,大致有纳米颗粒基底、纳米线基底等,不同的基底之间在增强机理和增强的效果之间有显著差别,现有技术中没有针对这些差别针对性的提供光学系统。However, the Raman scattering effect is a very weak process, so the Raman signal is very weak, and Raman spectroscopy studies of surface adsorbed species almost always use some kind of enhancement effect. In the prior art, the most common surface-enhanced Raman spectroscopy effect, the substrate of surface-enhanced Raman spectroscopy is the key technology, roughly including nanoparticle substrates, nanowire substrates, etc. The enhancement mechanism and enhancement effect between different substrates. There are significant differences between them, and there is no optical system specifically provided for these differences in the prior art.

发明内容SUMMARY OF THE INVENTION

鉴于现有技术中存在的问题,本发明提供了一种拉曼光谱成像方法,其特征在于:所述方法包括以下步骤:In view of the problems existing in the prior art, the present invention provides a Raman spectroscopy imaging method, characterized in that: the method comprises the following steps:

步骤(1)将检测对象分别置于纳米线阵列基底和纳米颗粒基底上;Step (1) placing the detection object on the nanowire array substrate and the nanoparticle substrate respectively;

步骤(2)当选择纳米线阵列基底时,光源发出的光依次经过所述纳米线阵列基底、第一物镜和成像单元;当选择纳米颗粒基底时,光源发出的光依次经过所述纳米颗粒基底、第二物镜和所述成像单元;Step (2) When the nanowire array substrate is selected, the light emitted by the light source passes through the nanowire array substrate, the first objective lens and the imaging unit in sequence; when the nanoparticle substrate is selected, the light emitted by the light source sequentially passes through the nanoparticle substrate , a second objective lens and the imaging unit;

步骤(3)所述成像单元将图像信息传输给上位机进行比较分析;In step (3), the imaging unit transmits the image information to the host computer for comparative analysis;

其中,所述第一物镜从物方到像方依次包括由正屈光度的第一透镜和负屈光度的第二透镜组成的第一胶合透镜、由正屈光度的第三透镜和负屈光度的第四透镜组成的第二胶合透镜以及负屈光度的第五透镜;Wherein, the first objective lens includes, from the object side to the image side, a first cemented lens composed of a first lens with positive refractive power and a second lens with negative refractive power, a third lens with positive refractive power and a fourth lens with negative refractive power composed of a second cemented lens and a fifth lens of negative diopter;

并满足d1/TTL>0.45,其中d1为所述所述第一透镜的半径,TTL为所述第一物镜的光学总长;and satisfy d 1 /TTL>0.45, wherein d 1 is the radius of the first lens, and TTL is the total optical length of the first objective lens;

所述第二物镜从物方到像方依次包括由正屈光度的第六透镜和负屈光度的第七透镜组成的第三胶合透镜、由正屈光度的第八透镜和负屈光度的第九透镜组成的第四胶合透镜以及负屈光度的第十透镜;The second objective lens sequentially includes a third cemented lens composed of a sixth lens with positive refractive power and a seventh lens with negative refractive power, and an eighth lens with positive refractive power and a ninth lens with negative refractive power in sequence from the object side to the image side. the fourth cemented lens and the tenth lens of negative diopter;

所述第二物镜的视场角θ满足,110°>θ>70°,所述第二物镜的数值孔径NA>0.6。The field of view angle θ of the second objective lens satisfies 110°>θ>70°, and the numerical aperture of the second objective lens NA>0.6.

优选地,所述第一物镜满足以下条件:1.9>f1/f40>1.2;Preferably, the first objective lens satisfies the following conditions: 1.9>f 1 /f 40 >1.2;

3.7>f1/f2>1.1;3.7>f 1 /f 2 >1.1;

5.1>f1/f3>2.4;5.1>f 1 /f 3 >2.4;

其中,所述第一胶合透镜的焦距为f1,所述第二胶合透镜的焦距为f2,所述第五透镜的焦距为f3,所述第一物镜的总焦距为f40The focal length of the first cemented lens is f 1 , the focal length of the second cemented lens is f 2 , the focal length of the fifth lens is f 3 , and the total focal length of the first objective lens is f 40 .

优选地,所述第二物镜满足以下条件:1.7>f5/f60>1.3;Preferably, the second objective lens satisfies the following conditions: 1.7>f 5 /f 60 >1.3;

2.7>f6/f60>1.5;2.7>f 6 /f 60 >1.5;

-1.2>f7/f60>-1.6;-1.2>f 7 /f 60 >-1.6;

其中,所述第三胶合透镜的焦距为f5,所述第四胶合透镜的焦距为f6,所述第十透镜的焦距为f7,所述第二物镜的总焦距为f60The focal length of the third cemented lens is f 5 , the focal length of the fourth cemented lens is f 6 , the focal length of the tenth lens is f 7 , and the total focal length of the second objective lens is f 60 .

本发明还提供了一种拉曼光谱成像装置,其特征在于:所述装置包括激光光源、对比选择单元、第一基底、第一物镜、第二基底、第二物镜以及成像单元;The present invention also provides a Raman spectrum imaging device, characterized in that: the device comprises a laser light source, a contrast selection unit, a first substrate, a first objective lens, a second substrate, a second objective lens and an imaging unit;

当所述对比选择单元选择第一基底时,所述光源发出的光依次经过所述第一基底、所述第一物镜和所述成像单元;其中第一基底是纳米线阵列基底;When the contrast selection unit selects the first substrate, the light emitted by the light source passes through the first substrate, the first objective lens and the imaging unit in sequence; wherein the first substrate is a nanowire array substrate;

当所述对比选择单元选择第二基底时,所述光源发出的光依次经过所述第二基底、所述第二物镜和所述成像单元;其中第二基底是纳米颗粒基底;When the contrast selection unit selects the second substrate, the light emitted by the light source passes through the second substrate, the second objective lens and the imaging unit in sequence; wherein the second substrate is a nanoparticle substrate;

所述第一物镜从物方到像方依次包括由正屈光度的第一透镜和负屈光度的第二透镜组成的第一胶合透镜、由正屈光度的第三透镜和负屈光度的第四透镜组成的第二胶合透镜以及负屈光度的第五透镜;The first objective lens includes, in order from the object side to the image side, a first cemented lens composed of a first lens with positive refractive power and a second lens with negative refractive power, a third lens with positive refractive power and a fourth lens with negative refractive power. The second cemented lens and the fifth lens of negative refractive power;

并满足d1/TTL>0.45,其中d1为所述所述第一透镜的半径,TTL为所述第一物镜的光学总长;and satisfy d 1 /TTL>0.45, wherein d 1 is the radius of the first lens, and TTL is the total optical length of the first objective lens;

所述第二物镜从物方到像方依次包括由正屈光度的第六透镜和负屈光度的第七透镜组成的第三胶合透镜、由正屈光度的第八透镜和负屈光度的第九透镜组成的第四胶合透镜以及负屈光度的第十透镜;The second objective lens sequentially includes a third cemented lens composed of a sixth lens with positive refractive power and a seventh lens with negative refractive power, and an eighth lens with positive refractive power and a ninth lens with negative refractive power in sequence from the object side to the image side. the fourth cemented lens and the tenth lens of negative diopter;

所述第二物镜的视场角θ满足,110°>θ>70°,所述第二物镜的数值孔径NA>0.6。The field of view angle θ of the second objective lens satisfies 110°>θ>70°, and the numerical aperture of the second objective lens NA>0.6.

优选地,所述第一基底和所述第二基底都位于样品台上,所述样品台可通过旋转来替换所述第一基底和所述第二基底,所述样品台还可在X、Y、Z三个方向上进行微调。Preferably, both the first substrate and the second substrate are located on a sample stage, the sample stage can be rotated to replace the first substrate and the second substrate, and the sample stage can also be used in X, Fine-tune in three directions of Y and Z.

与现有技术方案相比,本发明至少具有以下发明点及相应的有益效果:Compared with the prior art solutions, the present invention at least has the following invention points and corresponding beneficial effects:

(1)本发明根据纳米线基底和纳米颗粒基底的不同特性,针对性的设计了两组物镜,使用者可根据对象和基底的不同特性选择亦或是进行对比,该装置应用范围十分广泛。相比于现有技术,本发明针对的是纳米线和纳米颗粒的比较而对物镜进行了特别的设计。这一设计包括有对两种针对性的物镜的变换,采用了适于快速切换的旋转机构。该旋转机构可以在完成第一基底检测后快速切换成第二基底所需的物镜,这一点在纳米线和纳米颗粒的检测中非常重要。因为纳米线和纳米颗粒制备完成后需要快速完成检测,时间拖长,在封装前有引入杂质的风险,影响检测精度。因此使用例如旋转机构,利用旋转部件能够快速切换到所需的物镜,满足以上检测的需要。(1) According to the different characteristics of the nanowire substrate and the nanoparticle substrate, the present invention designs two groups of objective lenses. The user can select or compare according to the different characteristics of the object and the substrate. The device has a wide range of applications. Compared with the prior art, the present invention has specially designed the objective lens for the comparison of nanowires and nanoparticles. This design includes the transformation of two targeted objectives, using a rotating mechanism suitable for rapid switching. The rotating mechanism can quickly switch to the objective lens required for the second substrate after the detection of the first substrate is completed, which is very important in the detection of nanowires and nanoparticles. Because the nanowires and nanoparticles need to be tested quickly after the preparation is completed, the time is prolonged, and there is a risk of introducing impurities before packaging, which affects the detection accuracy. Therefore, using, for example, a rotating mechanism, the rotating component can be used to quickly switch to the desired objective lens, so as to meet the needs of the above detection.

(2)第一物镜组具体透镜的设计以及具体参数可最大化纳米线基底有效孔径大的优点。(2) The design and specific parameters of the specific lens of the first objective lens group can maximize the advantage of the large effective aperture of the nanowire substrate.

(3)第二物镜组具体透镜的设计以及具体参数针对纳米颗粒基底存在的缺陷,尽量提高分辨率,抑制该基底的缺陷。(3) The specific lens design and specific parameters of the second objective lens group are aimed at improving the resolution of the nanoparticle substrate and suppressing the defects of the substrate as much as possible.

需要提出的是,这一物镜是针对拉曼光谱而进行的特别设计,并不是采用其他领域的物镜所能代替的。这是因为拉曼光谱有其自身的特点,其需要适应的波长范围宽,同时还要满足成像的要求。另外,拉曼光散射角大,需要的物镜数值孔径也要大。上述但不仅限于上述的特点决定了物镜需要特别定制,并不是通用的物镜能完成基底检测需求的。It should be pointed out that this objective lens is specially designed for Raman spectroscopy, and cannot be replaced by objective lenses in other fields. This is because Raman spectroscopy has its own characteristics, and it needs to adapt to a wide range of wavelengths and at the same time meet the requirements of imaging. In addition, the large scattering angle of Raman light requires a large numerical aperture of the objective lens. The above-mentioned but not limited to the above-mentioned characteristics determine that the objective lens needs to be specially customized, and not a general-purpose objective lens can meet the requirements of substrate detection.

附图说明Description of drawings

图1是本发明提供的拉曼光谱成像装置的框架图;1 is a frame diagram of a Raman spectroscopy imaging device provided by the present invention;

图2是本发明第一物镜透镜组的结构图;Fig. 2 is the structure diagram of the first objective lens group of the present invention;

图3是本发明第一物镜场曲和畸变图;Fig. 3 is the field curvature and distortion diagram of the first objective lens of the present invention;

图4是本发明第一物镜色像差图;Fig. 4 is the first objective lens chromatic aberration diagram of the present invention;

图5是本发明第二物镜透镜组的结构图;Fig. 5 is the structure diagram of the second objective lens group of the present invention;

图6是本发明第二物镜镜场曲和畸变图;Fig. 6 is the field curvature and distortion diagram of the second objective lens of the present invention;

图7是本发明第二物镜色像差图;Fig. 7 is the chromatic aberration diagram of the second objective lens of the present invention;

图中:10、激光光源,20、对比选择单元,30、第一基底,40、第一物镜,50、第二基底,60、第二物镜,70、CCD成像单元,80、上位机,11、第一物镜第一透镜,12、第一物镜第二透镜,13、第一物镜第三透镜,第一物镜21、第一物镜第四透镜,3、第一物镜第五透镜,51、第二物镜第一透镜、52、第二物镜第二透镜,61、第二物镜第三透镜,62、第二物镜第四透镜,7、第二物镜第五透镜。In the figure: 10, laser light source, 20, contrast selection unit, 30, first substrate, 40, first objective lens, 50, second substrate, 60, second objective lens, 70, CCD imaging unit, 80, host computer, 11 , the first lens of the first objective lens, 12, the second lens of the first objective lens, 13, the third lens of the first objective lens, the first objective lens 21, the fourth lens of the first objective lens, 3, the fifth lens of the first objective lens, 51, the first Two objective lenses, the first lens, 52, the second lens of the second objective, 61, the third lens of the second objective, 62, the fourth lens of the second objective, and 7, the fifth lens of the second objective.

下面对本发明进一步详细说明。但下述的实例仅仅是本发明的简易例子,并不代表或限制本发明的权利保护范围,本发明的保护范围以权利要求书为准。The present invention will be described in further detail below. However, the following examples are only simple examples of the present invention, and do not represent or limit the protection scope of the present invention. The protection scope of the present invention is subject to the claims.

具体实施方式Detailed ways

下面结合附图并通过具体实施方式来进一步说明本发明的技术方案。The technical solutions of the present invention are further described below with reference to the accompanying drawings and through specific embodiments.

为更好地说明本发明,便于理解本发明的技术方案,本发明的典型但非限制性的实施例如下:In order to better illustrate the present invention and facilitate the understanding of the technical solutions of the present invention, typical but non-limiting examples of the present invention are as follows:

实施例1Example 1

在本实施例中,如图1所示,拉曼光谱成像装置包括激光光源10、对比选择单元20、第一基底30、第一物镜40、第二基底50、第二物镜60、CCD成像单元70以及上位机80。In this embodiment, as shown in FIG. 1 , the Raman spectral imaging device includes a laser light source 10 , a contrast selection unit 20 , a first substrate 30 , a first objective lens 40 , a second substrate 50 , a second objective lens 60 , and a CCD imaging unit 70 and the host computer 80.

其中当对比选择单元20选择第一基底30来承载样品时,激光光源10发出的光线经过第一基底30,再依次通过第一物镜40、最终光线达到CCD成像单元,并将图像信息传输给上位机进行存储;When the comparison selection unit 20 selects the first substrate 30 to carry the sample, the light emitted by the laser light source 10 passes through the first substrate 30, then passes through the first objective lens 40 in turn, and finally the light reaches the CCD imaging unit, and transmits the image information to the upper position. machine for storage;

当对比选择单元20选择第二基底50来承载样品时,激光光源10发出的光线经过第二基底50,再依次通过第二物镜60、最终光线达到CCD成像单元,并将图像信息传输给上位机进行存储。When the comparison selection unit 20 selects the second substrate 50 to carry the sample, the light emitted by the laser light source 10 passes through the second substrate 50, then passes through the second objective lens 60 in turn, and finally the light reaches the CCD imaging unit, and transmits the image information to the host computer to store.

需要指出的是,第一基底30检测完成后,可以利用物镜转换装置例如旋转机构快速完成物镜从第一物镜40切换成第二物镜60,这样对于刚制备出的需要快速检测的基底特别适用。这样可以避免因等待第二物镜60的调试而造成基底材料在封装前引入杂质的风险。It should be pointed out that after the detection of the first substrate 30 is completed, the objective lens can be quickly switched from the first objective lens 40 to the second objective lens 60 by using an objective lens conversion device such as a rotating mechanism, which is especially suitable for newly prepared substrates that require rapid detection. In this way, the risk of introducing impurities into the base material before encapsulation due to waiting for the commissioning of the second objective lens 60 can be avoided.

对比选择单元20可以根据被检测材料的具体性质,结合纳米线基底和纳米颗粒基底的特性,来选择第一物镜40或是第二物镜60,也可用同一种样品分别在第一物镜40和第二物镜60下进行检测,对被检测对象和基底材料做进一步的科学研究。The contrast selection unit 20 can select the first objective lens 40 or the second objective lens 60 according to the specific properties of the detected material and the characteristics of the nanowire substrate and the nanoparticle substrate. Detected under two objective lenses 60, and further scientific research on the detected object and base material.

其中第一基底30是在硅衬底上形成高质量的金属纳米线阵列,其中金属可以是金、银或铜等贵金属;其中纳米线为规律的周期性结构,当采用的激光光源的波长略大于上述纳米线的周期,入射的点光源的能量耦合到表面等离子体波上,显著的增大出射的有效孔径光阑。The first substrate 30 is a high-quality metal nanowire array formed on a silicon substrate, wherein the metal can be a precious metal such as gold, silver or copper; wherein the nanowire is a regular periodic structure, when the wavelength of the laser light source used is slightly Greater than the period of the above nanowire, the energy of the incident point light source is coupled to the surface plasmon wave, and the outgoing effective aperture stop is significantly increased.

对应第一基底30,特设计第一物镜40具体如下:从物方到像方依次包括具有正折射率的第一透镜11、具有负折射率的第二透镜12、具有正折射率的第三透镜21、具有负折射率的第四透镜22、具有负折射率的第五透镜3;其中第一透镜11和第二透镜12是胶合透镜,第三透镜21和第四透镜22是胶合透镜,其中通过两个正负透镜组合而成的胶合透镜,最大程度的减小了色差;各透镜参数如下:Corresponding to the first substrate 30, the specially designed first objective lens 40 is specifically as follows: from the object side to the image side, it includes a first lens 11 with a positive refractive index, a second lens 12 with a negative refractive index, and a third lens with a positive refractive index. lens 21, fourth lens 22 with negative refractive index, fifth lens 3 with negative refractive index; wherein the first lens 11 and the second lens 12 are cemented lenses, the third lens 21 and the fourth lens 22 are cemented lenses, Among them, the cemented lens formed by the combination of two positive and negative lenses minimizes chromatic aberration; the parameters of each lens are as follows:

表一:纳米线基底物镜参数Table 1: Nanowire Substrate Objective Lens Parameters

Figure GDA0003808297490000071
Figure GDA0003808297490000071

如图3所示,本发明第一物镜的场曲图和畸变图;As shown in Figure 3, the field curvature and distortion diagram of the first objective lens of the present invention;

如图4所示,本发明第一物镜的色像差图;As shown in Figure 4, the chromatic aberration diagram of the first objective lens of the present invention;

此外,第一透镜11、第二透镜12的透镜半径是d1,第一物镜的光学系统总长为TTL,d1/TTL>0.45,使得第一物镜具有较大的有效孔径,在该实施例中,第一透镜11、第二透镜12的透镜半径d1=5mm,光学系统总长为TTL为9mm;In addition, the lens radius of the first lens 11 and the second lens 12 is d1, the total length of the optical system of the first objective lens is TTL, and d 1 /TTL>0.45, so that the first objective lens has a larger effective aperture. In this embodiment , the lens radius d 1 of the first lens 11 and the second lens 12 is 5mm, and the total length of the optical system is TTL of 9mm;

第一物镜中第一透镜11和第二透镜12组成的胶合透镜的焦距为f1,第三透镜21和第四透镜22组成的胶合透镜的焦距为f2,第五透镜3的焦距为f3,第一物镜的总焦距为f40,以上各焦距满足以下关系:In the first objective lens, the focal length of the cemented lens composed of the first lens 11 and the second lens 12 is f 1 , the focal length of the cemented lens composed of the third lens 21 and the fourth lens 22 is f 2 , and the focal length of the fifth lens 3 is f 3. The total focal length of the first objective lens is f 40 , and the above focal lengths satisfy the following relationship:

1.9>f1/f40>1.2;1.9>f 1 /f 40 >1.2;

3.7>f1/f2>1.1;3.7>f 1 /f 2 >1.1;

5.1>f1/f3>2.4。5.1>f 1 /f 3 >2.4.

其中第二基底50是在硅衬底上形成高质量的纳米颗粒薄膜,其中金属可以是金、银或铜等贵金属;由于纳米颗粒的尺寸较小,会发生只出现电偶极子共振模式的情况,光谱上出现一个SPR峰,当颗粒的尺寸增加时,该SPR峰红移,在短波区域出现新的高阶的SPR峰,但是,在一般情况下,这些共振峰有相当的光谱宽度,彼此之间会互相重叠,各自所占的比例不好区分.在某些特殊情况下,有些共振峰不太好辨认其物理根源。Wherein the second substrate 50 is a high-quality nanoparticle film formed on a silicon substrate, wherein the metal can be a precious metal such as gold, silver or copper; due to the small size of the nanoparticles, only the electric dipole resonance mode will occur. In the case, an SPR peak appears on the spectrum. When the size of the particles increases, the SPR peak redshifts, and new high-order SPR peaks appear in the short-wave region, but, in general, these resonance peaks have a comparable spectral width, They will overlap with each other, and their respective proportions are difficult to distinguish. In some special cases, some formants are not easy to identify their physical origins.

对应第二基底50,特设计第二物镜60具体如下:Corresponding to the second substrate 50, the specially designed second objective lens 60 is as follows:

特设计第二物镜具体如下:从物方到像方依次包括具有正折射率的第一透镜51、具有负折射率的第二透镜52、具有正折射率的第三透镜61、具有负折射率的第四透镜62、具有负折射率的第五透镜7;其中第一透镜51和第二透镜52是胶合透镜,第三透镜61和第四透镜62是胶合透镜,其中通过两个正负透镜组合而成的胶合透镜,最大程度的减小了色差;各透镜参数如下:The specially designed second objective lens is as follows: from the object side to the image side, it sequentially includes a first lens 51 with a positive refractive index, a second lens 52 with a negative refractive index, a third lens 61 with a positive refractive index, and a negative refractive index lens 61. The fourth lens 62, the fifth lens 7 having a negative refractive index; wherein the first lens 51 and the second lens 52 are cemented lenses, the third lens 61 and the fourth lens 62 are cemented lenses, wherein through two positive and negative lenses The combined cemented lens minimizes chromatic aberration; the parameters of each lens are as follows:

表二:纳米颗粒基底物镜参数Table 2: Nanoparticle Substrate Objective Lens Parameters

Figure GDA0003808297490000091
Figure GDA0003808297490000091

如图6所示,本发明第二物镜的场曲图和畸变图;As shown in Figure 6, the field curvature and distortion diagram of the second objective lens of the present invention;

如图7所示,本发明第二物镜的色像差图;As shown in Figure 7, the chromatic aberration diagram of the second objective lens of the present invention;

其中第二物镜的视场角θ满足,110°>θ>70°,第二物镜的数值孔径NA>0.6,使得透镜组具有高分辨率;The field angle θ of the second objective lens satisfies, 110°>θ>70°, and the numerical aperture of the second objective lens NA>0.6, so that the lens group has high resolution;

第二物镜中第一透镜51和第二透镜52组成的胶合透镜的焦距为f5,第三透镜61和第四透镜62组成的胶合透镜的焦距为f6,第五透镜7的焦距为f7,第二物镜的总焦距为f60,以上各焦距满足以下关系:In the second objective lens, the focal length of the cemented lens composed of the first lens 51 and the second lens 52 is f 5 , the focal length of the cemented lens composed of the third lens 61 and the fourth lens 62 is f 6 , and the focal length of the fifth lens 7 is f 7. The total focal length of the second objective lens is f 60 , and the above focal lengths satisfy the following relationship:

1.7>f5/f60>1.3;1.7>f 5 /f 60 >1.3;

2.7>f6/f60>1.5;2.7>f 6 /f 60 >1.5;

-1.2>f7/f60>-1.6。-1.2>f 7 /f 60 >-1.6.

在上述光谱成像装置中,第一基底和第二基底都位于样品台(图中未示出)上,所述样品台可通过旋转来替换第一基底和第二基底,所述样品台还可在X、Y、Z三个方向上根据使用者的需要进行微调,以应对不同的物镜的不同焦距和/或对准检测样品、调整检测样品的角度。In the above spectroscopic imaging device, both the first substrate and the second substrate are located on a sample stage (not shown in the figure), the sample stage can be rotated to replace the first substrate and the second substrate, and the sample stage can also In the three directions of X, Y, and Z, it can be fine-tuned according to the needs of the user to cope with the different focal lengths of different objective lenses and/or to align and adjust the angle of the test sample.

申请人声明,本发明通过上述实施例来说明本发明的详细结构特征,但本发明并不局限于上述详细结构特征,即不意味着本发明必须依赖上述详细结构特征才能实施。所属技术领域的技术人员应该明了,对本发明的任何改进,对本发明所选用部件的等效替换以及辅助部件的增加、具体方式的选择等,均落在本发明的保护范围和公开范围之内。The applicant declares that the present invention illustrates the detailed structural features of the present invention through the above embodiments, but the present invention is not limited to the above detailed structural features, that is, it does not mean that the present invention must rely on the above detailed structural features to be implemented. Those skilled in the art should understand that any improvement to the present invention, the equivalent replacement of the selected components of the present invention, the addition of auxiliary components, the selection of specific methods, etc., all fall within the protection scope and disclosure scope of the present invention.

以上详细描述了本发明的优选实施方式,但是,本发明并不限于上述实施方式中的具体细节,在本发明的技术构思范围内,可以对本发明的技术方案进行多种简单变型,这些简单变型均属于本发明的保护范围。The preferred embodiments of the present invention are described in detail above, but the present invention is not limited to the specific details of the above-mentioned embodiments. Within the scope of the technical concept of the present invention, various simple modifications can be made to the technical solutions of the present invention. These simple modifications All belong to the protection scope of the present invention.

另外需要说明的是,在上述具体实施方式中所描述的各个具体技术特征,在不矛盾的情况下,可以通过任何合适的方式进行组合,为了避免不必要的重复,本发明对各种可能的组合方式不再另行说明。In addition, it should be noted that the specific technical features described in the above-mentioned specific embodiments can be combined in any suitable manner unless they are inconsistent. In order to avoid unnecessary repetition, the present invention provides The combination method will not be specified otherwise.

此外,本发明的各种不同的实施方式之间也可以进行任意组合,只要其不违背本发明的思想,其同样应当视为本发明所公开的内容。In addition, the various embodiments of the present invention can also be combined arbitrarily, as long as they do not violate the spirit of the present invention, they should also be regarded as the contents disclosed in the present invention.

Claims (3)

1. A Raman spectrum imaging method is characterized in that: the method comprises the following steps:
respectively placing detection objects on a nanowire array substrate and a nanoparticle substrate;
when the nanowire array substrate is selected, light emitted by a light source sequentially passes through the nanowire array substrate, a first objective lens and an imaging unit; when the nanoparticle substrate is selected, light emitted by the light source sequentially passes through the nanoparticle substrate, the second objective lens and the imaging unit;
the imaging unit transmits the image information to an upper computer for comparison and analysis;
the first objective lens comprises a first cemented lens consisting of a first lens with positive diopter and a second lens with negative diopter, a second cemented lens consisting of a third lens with positive diopter and a fourth lens with negative diopter and a fifth lens with negative diopter in sequence from the object space to the image space;
and satisfy d 1 /TTL>0.45, wherein d 1 TTL is the optical total length of the first objective lens and is the radius of the first lens;
the second objective lens sequentially comprises a third cemented lens consisting of a sixth lens with positive diopter and a seventh lens with negative diopter, a fourth cemented lens consisting of an eighth lens with positive diopter and a ninth lens with negative diopter and a tenth lens with negative diopter from the object side to the image side;
the field angle theta of the second objective lens meets the condition that 110 degrees > theta >70 degrees, and the numerical aperture NA of the second objective lens is >0.6;
the first objective lens satisfies the following condition: 1.9>f 1 /f 40 >1.2;
3.7>f 1 /f 2 >1.1;
5.1>f 1 /f 3 >2.4;
Wherein the focal length of the first cemented lens is f 1 The focal length of the second cemented lens is f 2 A focal length f of the fifth lens 3 The total focal length of the first objective lens is f 40
The second objective lens satisfies the following conditions: 1.7>f 5 /f 60 >1.3;
2.7>f 6 /f 60 >1.5;
-1.2>f 7 /f 60 >-1.6;
Wherein the third cemented lens has a focal length f 5 A focal length f of the fourth cemented lens 6 A focal length of the tenth lens is f 7 The total focal length of the second objective lens is f 60
2. A raman spectral imaging device characterized by: the device comprises a laser light source, a contrast selection unit, a first substrate, a first objective lens, a second substrate, a second objective lens and an imaging unit;
when the contrast selection unit selects a first substrate, light emitted by the light source sequentially passes through the first substrate, the first objective lens and the imaging unit; wherein the first substrate is a nanowire array substrate;
when the contrast selection unit selects a second substrate, light emitted by the light source sequentially passes through the second substrate, the second objective lens and the imaging unit; wherein the second substrate is a nanoparticle substrate;
the first objective lens comprises a first cemented lens consisting of a first lens with positive diopter and a second lens with negative diopter, a second cemented lens consisting of a third lens with positive diopter and a fourth lens with negative diopter and a fifth lens with negative diopter in sequence from the object space to the image space;
and satisfy d 1 /TTL>0.45, wherein d 1 The radius of the first lens is defined, and TTL is the total optical length of the first objective lens;
the second objective lens sequentially comprises a third cemented lens consisting of a sixth lens with positive diopter and a seventh lens with negative diopter, a fourth cemented lens consisting of an eighth lens with positive diopter and a ninth lens with negative diopter and a tenth lens with negative diopter from the object space to the image space;
the field angle theta of the second objective lens meets the condition that 110 degrees > theta >70 degrees, and the numerical aperture NA of the second objective lens is >0.6;
the first objective lens satisfies the following condition: 1.9>f 1 /f 40 >1.2;
3.7>f 1 /f 2 >1.1;
5.1>f 1 /f 3 >2.4;
Wherein, the first stepA cemented lens having a focal length of f 1 The focal length of the second cemented lens is f 2 A focal length f of the fifth lens 3 The total focal length of the first objective lens is f 40
The second objective lens satisfies the following conditions: 1.7>f 5 /f 60 >1.3;
2.7>f 6 /f 60 >1.5;
-1.2>f 7 /f 60 >-1.6;
Wherein the third cemented lens has a focal length f 5 A focal length f of the fourth cemented lens 6 A focal length of the tenth lens is f 7 The total focal length of the second objective lens is f 60
3. The apparatus of claim 2, wherein: the first base and the second base are both positioned on a sample stage, the first base and the second base can be replaced by the sample stage through rotation, and the sample stage can be finely adjusted in three directions of X, Y and Z.
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