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CN110501319A - Raman super-resolution microscopy imaging method with multi-channel structured light illumination - Google Patents

Raman super-resolution microscopy imaging method with multi-channel structured light illumination Download PDF

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CN110501319A
CN110501319A CN201910807953.1A CN201910807953A CN110501319A CN 110501319 A CN110501319 A CN 110501319A CN 201910807953 A CN201910807953 A CN 201910807953A CN 110501319 A CN110501319 A CN 110501319A
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王宏达
孙佳音
初宏亮
吴强
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Changchun Institute of Applied Chemistry of CAS
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    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • 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
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    • G01N21/645Specially adapted constructive features of fluorimeters
    • G01N21/6456Spatial resolved fluorescence measurements; Imaging
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Abstract

多通路结构光照明拉曼超分辨显微成像方法,涉及微观粒子超分辨成像技术领域,在现有的结构光超分辨显微系统的成像光路中,加入拉曼分光成像模块,通过多种拉曼探针的选取,实现复杂体系中不同观测物的特异性成像。包括激发光模块、结构光照明模块和拉曼分光成像模块;选取特定的拉曼探针分子,将所述拉曼探针分子与抗体结合,对被测样品进行特异性标记;开启激发光模块,以倒置荧光显微镜为平台,结构光照明模块出射的光条纹激发被测样品;被激发出来探针的信号通过拉曼分光成像模块实现信号的特异性分选,然后在CCD处成像。本发明可用于内吞/转运单个分子及颗粒体系、病毒进入细胞机理、活细胞内分子的动态过程等研究方向。

The multi-channel structured light illumination Raman super-resolution microscopy imaging method relates to the technical field of microscopic particle super-resolution imaging. In the imaging light path of the existing structured light super-resolution microscopy system, a Raman spectroscopic imaging module is added, and a Raman spectroscopic imaging module is added to the imaging light path of the existing structured light super-resolution microscopy system, and through a variety of imaging methods The selection of Mann probes enables specific imaging of different objects in complex systems. It includes an excitation light module, a structured light illumination module and a Raman spectroscopic imaging module; select a specific Raman probe molecule, combine the Raman probe molecule with an antibody, and specifically label the sample to be tested; turn on the excitation light module , using an inverted fluorescence microscope as a platform, the light stripes emitted by the structured light illumination module excite the tested sample; the signals of the excited probes are specifically sorted by the Raman spectroscopic imaging module, and then imaged at the CCD. The invention can be used in research directions such as endocytosis/transport of single molecules and particle systems, the mechanism of virus entry into cells, and the dynamic process of molecules in living cells.

Description

多通路结构光照明的拉曼超分辨显微成像方法Raman super-resolution microscopy imaging method with multi-channel structured light illumination

技术领域technical field

本发明涉及微观粒子超分辨成像技术领域,具体涉及一种多通路结构光照明拉曼超分辨显微成像方法。The invention relates to the technical field of microscopic particle super-resolution imaging, in particular to a multi-channel structured light illumination Raman super-resolution microscopic imaging method.

背景技术Background technique

结构光照明超分辨荧光显微技术(SIM)是近几年发展来的一种新型的超分辨宽场成像技术。SIM超分辨技术以普通的倒置荧光显微镜为平台,利用特定的激发光路产生空间频率已知的正弦条纹,对样品进行荧光信号的激发,对采集到的信号进行数据的分离与重构,可获得具有二倍衍射极限的超分辨成像。SIM超分辨技术成像速度较快,不需要长时间、大量的采集样品信息,适用于活体细胞的成像分析。Structured light illumination super-resolution fluorescence microscopy (SIM) is a new type of super-resolution wide-field imaging technology developed in recent years. SIM super-resolution technology takes an ordinary inverted fluorescence microscope as a platform, uses a specific excitation light path to generate sinusoidal fringes with a known spatial frequency, excites the fluorescence signal of the sample, and separates and reconstructs the collected signal data. Super-resolution imaging with twice the diffraction limit. SIM super-resolution technology has a fast imaging speed, does not require a long time and a large amount of sample information collection, and is suitable for imaging analysis of living cells.

光学探针是研究复杂生物系统中特定目标的有效工具。基于拉曼散射的拉曼探针,谱线十分锐利、分辨率高、特异性强。此外,水的拉曼信号很弱,拉曼探针可在水环境样品中进行直接检测。但是拉曼探针也有它的不足之处,就是它的信号强度较低(比荧光信号低两个数量级)。通过表面增强拉曼(SERS)探针以及共振拉曼(PR)探针标记的方法,能够将拉曼信号的强度提高102-106,可解决拉曼信号强度低的问题。综上,对于生物样品而言,尤其是活体细胞的观测,用拉曼探针进行特异性标记成像,是一种理想的分析手段。Optical probes are effective tools for studying specific targets in complex biological systems. Raman probes based on Raman scattering have very sharp spectral lines, high resolution and strong specificity. In addition, the Raman signal of water is very weak, and Raman probes can be directly detected in water environmental samples. But the Raman probe also has its disadvantage, that is, its signal intensity is low (two orders of magnitude lower than the fluorescent signal). The Raman signal intensity can be increased by 10 2 -10 6 through the method of surface-enhanced Raman (SERS) probe and resonance Raman (PR) probe labeling, which can solve the problem of low Raman signal intensity. To sum up, for biological samples, especially the observation of living cells, using Raman probes for specific labeling imaging is an ideal analysis method.

细胞的荧光显微镜图像能显示荧光标记的分子,让研究人员实时观察活细胞或固定样品内特殊分子或蛋白复合物的运动,但荧光信号的特异性较差,无法满足复杂体系下观察某种(或某几种)特定目标的研究需求,此外,荧光标记的体积相对较大,在标记生物小分子时会改变其生物活性,但是相对于拉曼信号而言,荧光信号的强度较高,较易被相机采集。Fluorescence microscope images of cells can display fluorescently labeled molecules, allowing researchers to observe the movement of special molecules or protein complexes in living cells or fixed samples in real time, but the specificity of fluorescent signals is poor and cannot meet the requirements of observing certain ( Or some kinds of research needs of specific targets, in addition, the volume of fluorescent labeling is relatively large, which will change its biological activity when labeling small biological molecules, but compared with the Raman signal, the intensity of the fluorescent signal is higher, which is relatively large. Easy to be captured by camera.

发明内容SUMMARY OF THE INVENTION

本发明提供了一种多通路结构光照明拉曼超分辨显微成像方法,在现有的结构光超分辨显微系统的成像光路中,加入拉曼分光成像模块,通过多种拉曼探针的选取,实现复杂体系中不同观测物的特异性成像。The invention provides a multi-channel structured light illumination Raman super-resolution microscopy imaging method. In the imaging light path of the existing structured light super-resolution microscopy system, a Raman spectroscopic imaging module is added, and a Raman spectroscopic imaging module is added to pass through various Raman probes. The choice of , to achieve specific imaging of different objects in complex systems.

多通路结构光照明拉曼超分辨显微成像方法,其特征是;包括成像系统,所述成像系统包括激发光模块、结构光照明模块和拉曼分光成像模块;该方法由以下步骤实现:The multi-channel structured light illumination Raman super-resolution microscopy imaging method is characterized by comprising an imaging system including an excitation light module, a structured light illumination module and a Raman spectroscopic imaging module; the method is realized by the following steps:

步骤一、选取特定的拉曼探针分子,将所述拉曼探针分子与抗体结合,对被测样品进行特异性标记;Step 1: Select a specific Raman probe molecule, combine the Raman probe molecule with an antibody, and specifically label the sample to be tested;

步骤二、开启激发光模块,以倒置荧光显微镜为平台,所述结构光照明模块出射的光条纹激发被测样品;Step 2: Turn on the excitation light module, take the inverted fluorescence microscope as a platform, and the light stripes emitted by the structured light illumination module excite the sample to be tested;

步骤三、被激发出来探针的信号通过拉曼分光成像模块实现信号的特异性分选,然后在CCD处成像,重构获得具有二倍衍射极限的超分辨成像。Step 3: The signals of the excited probes are specifically sorted by the Raman spectroscopic imaging module, and then imaged at the CCD, and reconstructed to obtain super-resolution imaging with twice the diffraction limit.

本发明的有益效果:Beneficial effects of the present invention:

本发明提供多通路结构光照明拉曼超分辨显微成像方法,选取了488、532、633、785nm四个波长的激光器,可满足不同探针对激发波长的需求;The invention provides a multi-channel structured light illumination Raman super-resolution microscopic imaging method, and four wavelengths of 488, 532, 633, and 785 nm lasers are selected, which can meet the excitation wavelength requirements of different probes;

本发明提供多通路结构光照明拉曼超分辨显微成像方法,将拉曼探针标记技术与结构光超分辨成像技术相结合,能够实现特异性超分辨成像,提高了宽场拉曼成像的分辨率;The invention provides a multi-channel structured light illumination Raman super-resolution microscopic imaging method, which combines the Raman probe labeling technology with the structured light super-resolution imaging technology, can realize specific super-resolution imaging, and improves the performance of wide-field Raman imaging. resolution;

本发明提供多通路结构光照明拉曼超分辨显微成像方法,采用拉曼分光成像模块对不同探针的特征峰值信号进行选通,系统稳定性高,成像速度快;The invention provides a multi-channel structured light illumination Raman super-resolution microscopic imaging method, which adopts a Raman spectroscopic imaging module to gate the characteristic peak signals of different probes, and has high system stability and fast imaging speed;

本发明提供多通路结构光照明拉曼超分辨显微成像方法,对样品制备的要求较低,较适用于活体细胞的观察研究,能用于内吞/转运单个分子及颗粒体系、病毒进入细胞机理、活细胞内分子的动态过程等研究方向。The invention provides a multi-channel structured light illumination Raman super-resolution microscopic imaging method, which has lower requirements for sample preparation, is more suitable for observation and research of living cells, and can be used for endocytosis/transport of single molecules and particle systems, and virus entry into cells Mechanism, dynamic process of molecules in living cells and other research directions.

附图说明Description of drawings

图1为本发明所述的多通路结构光照明拉曼超分辨显微成像方法中单模光纤耦合的多通路激发光模块示意图;1 is a schematic diagram of a multi-channel excitation light module coupled with a single-mode fiber in the multi-channel structured light illumination Raman super-resolution microscopy imaging method according to the present invention;

图2为本发明所述的多通路结构光照明拉曼超分辨显微成像方法中结构光照明模块示意图;2 is a schematic diagram of a structured light illumination module in the multi-channel structured light illumination Raman super-resolution microscopy imaging method according to the present invention;

图3为本发明所述的多通路结构光照明拉曼超分辨显微成像方法中拉曼分光成像模块示意图;3 is a schematic diagram of a Raman spectroscopic imaging module in the multi-channel structured light illumination Raman super-resolution microscopy imaging method according to the present invention;

图4为本发明所述的多通路结构光照明拉曼超分辨显微成像方法中成像系统的整体光路结构图;4 is an overall optical path structure diagram of an imaging system in the multi-channel structured light illumination Raman super-resolution microscopy imaging method according to the present invention;

图5为本发明所述的多通路结构光照明拉曼超分辨显微成像方法中的流程图。FIG. 5 is a flowchart of the multi-channel structured light illumination Raman super-resolution microscopy imaging method according to the present invention.

具体实施方式Detailed ways

具体实施方式一、结合图1至图5说明本实施方式,多通路结构光照明拉曼超分辨显微成像方法,该成像方法中包括成像系统,所述成像系统包括激发光模块、结构光照明模块和拉曼分光成像模块;所述激发光模块包括488nm、532nm、633nm以及785nm波长的激光器、耦合器1和单模光纤2;所述结构光照明模块包括准直器3、声光调制器4、扩束镜组5、半波片6、PBS分束器7、铁电液晶8、第一组透镜9、普克尔盒10、反射镜11、第二组透镜12、第一汇聚镜13、掩模板14、准直镜15和第二汇聚镜16;所述拉曼分光成像模块包括管镜17、载有滤波片的电动转轮18和CCD;DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS First, the present embodiment will be described with reference to FIG. 1 to FIG. 5 , a multi-channel structured light illumination Raman super-resolution microscopy imaging method, the imaging method includes an imaging system, and the imaging system includes an excitation light module, a structured light illumination module and Raman spectroscopic imaging module; the excitation light module includes lasers with wavelengths of 488 nm, 532 nm, 633 nm and 785 nm, a coupler 1 and a single-mode fiber 2; the structured light illumination module includes a collimator 3, an acousto-optic modulator 4. Beam expander group 5, half-wave plate 6, PBS beam splitter 7, ferroelectric liquid crystal 8, first group lens 9, Pockels cell 10, reflector 11, second group lens 12, first converging mirror 13. The mask plate 14, the collimating mirror 15 and the second converging mirror 16; the Raman spectroscopic imaging module includes a tube mirror 17, a motorized runner 18 carrying a filter, and a CCD;

所述488nm、532nm、633nm、785nm波长的激光器经由各自对应的二向色镜反(透)射汇聚于耦合器1处,后由耦合器耦合至单模光纤2中。The lasers with wavelengths of 488 nm, 532 nm, 633 nm, and 785 nm are reflected (transmitted) at the coupler 1 through the corresponding dichroic mirrors, and then coupled into the single-mode fiber 2 by the coupler.

单模光纤耦合出射的发散光束首先经过准直器3准直;再由声光调制器4在上述四种激发波长中进行遴选;后由扩束镜组5对光束口径进行扩大;而后通过半波片6将光束偏振态调节为S方向;进一步经过PBS分束器7,将S方向的光束反射至铁电液晶8上,通过对铁电液晶像素的加载,可以将一束光衍射成多束出射;为了适合普克尔盒10的通光口径,在其前后分别放置第一组透镜9以及第二组透镜12,使得光束无阻碍地普克尔盒,而普克尔盒的作用则是对出射光束的偏振方向进行调制,以保证干涉条纹具有最佳的对比度;反射镜11,在系统中的作用是转折光束,以压缩整个系统的长度;调制好偏振态的光束通过第一汇聚镜13,到达掩模板14,掩模板14上打有6个孔洞,这些孔洞对应着平面内三个不同的照明方向下±1级光束汇聚的空间位置,能够滤除0级光束以及其它高级次衍射光;光束进一步向前传播,先后通过15)准直镜的准直以及第二汇聚镜16的聚焦,而后进入倒置荧光显微镜,最后在物镜的焦平面处实现结构光照明。The divergent beam coupled out of the single-mode fiber is firstly collimated by the collimator 3; then selected from the above four excitation wavelengths by the acousto-optic modulator 4; then the beam diameter is expanded by the beam expander group 5; The wave plate 6 adjusts the polarization state of the beam to the S direction; further, through the PBS beam splitter 7, the beam in the S direction is reflected to the ferroelectric liquid crystal 8. By loading the ferroelectric liquid crystal pixel, a beam of light can be diffracted into multiple The beam exits; in order to fit the clear aperture of the Pockels cell 10, the first group of lenses 9 and the second group of lenses 12 are placed before and after it, so that the light beam is unobstructed in the Pockels box, and the function of the Pockels box is is to modulate the polarization direction of the outgoing beam to ensure that the interference fringes have the best contrast; the function of the mirror 11 in the system is to turn the beam to compress the length of the entire system; the modulated polarization state of the beam passes through the first convergence The mirror 13 reaches the mask plate 14. There are 6 holes on the mask plate 14. These holes correspond to the spatial positions of the ±1-level beams in three different illumination directions in the plane, which can filter out the 0-level beams and other high-level beams. Diffracted light; the light beam further propagates forward, successively passes through 15) the collimation of the collimating lens and the focusing of the second converging mirror 16, and then enters the inverted fluorescence microscope, and finally realizes structured light illumination at the focal plane of the objective lens.

图3为拉曼分光成像模块示意图。样品激发出来的拉曼(荧光)信号先经由管镜17,再进一步向前传播至载有不同中心波长窄带滤光片(例如,Semrock FF01-575/5-25、FF01-680/13-25型滤光片等)的电动转轮18。窄带滤光片的中心波长与拉曼探针的拉曼特征峰值相对应,它的作用是能够将其它背景信号滤除,仅使所需的特异性拉曼信号通过。拉曼信号进一步向前传播到达CCD相机,参与数据的采集。而当系统进行荧光成像时,转轮可转到空位置,使得荧光信号通过。滤光片转轮的采用,提高了系统的成像速度,非扫描的一次性成像方式,也大大降低了系统的不稳定性。通过不同探针标记的不同观测目标激发出来的特征信号,可以对复杂体系下的多个观测目标进行特异性快速超分辨成像。FIG. 3 is a schematic diagram of a Raman spectroscopic imaging module. The Raman (fluorescence) signal excited by the sample first passes through the tube lens 17, and then further forwards to narrow-band filters with different center wavelengths (eg, Semrock FF01-575/5-25, FF01-680/13-25 type filter, etc.) of the motorized wheel 18. The central wavelength of the narrow-band filter corresponds to the Raman characteristic peak of the Raman probe, and its function is to filter out other background signals and only pass the desired specific Raman signal. The Raman signal further propagates forward to the CCD camera and participates in data acquisition. When the system is performing fluorescence imaging, the wheel can be turned to the empty position, allowing the fluorescence signal to pass through. The use of the filter wheel improves the imaging speed of the system, and the non-scanning one-time imaging method also greatly reduces the instability of the system. Through the characteristic signals excited by different observation targets labeled with different probes, specific and fast super-resolution imaging can be performed on multiple observation targets in a complex system.

在拉曼分光成像模块中,也兼具荧光成像的功能,使得拉曼探针与荧光探针实现使用范围上的互补。由于探针是具有波长选择性的,因此,系统以多通路激发光模块作为拉曼信号的激发光源。In the Raman spectroscopic imaging module, it also has the function of fluorescence imaging, so that the Raman probe and the fluorescent probe can be used to complement each other. Since the probe is wavelength-selective, the system uses a multi-channel excitation light module as the excitation light source for Raman signals.

本实施方式中,结合图4的成像系统结构图,基于各个模块的多通路结构光照明超分辨拉曼显微成像方法,能够实现复杂体系下,多种目标成分的超分辨显微成像分析,成像速度快,可靠性强,此外,该成像方法还可通过改变或优化其中的某一模块以满足不同应用领域的需求,具有较强的灵活性和广泛的适用性。In this embodiment, combined with the imaging system structure diagram in FIG. 4 , the multi-channel structured light illumination super-resolution Raman microscopy imaging method based on each module can realize the super-resolution microscopy imaging analysis of various target components in a complex system, The imaging speed is fast and the reliability is strong. In addition, the imaging method can also meet the needs of different application fields by changing or optimizing one of the modules, and has strong flexibility and wide applicability.

结合图5说明本实施方式,本实施方式的成像方法具体由以下步骤实现:This embodiment is described with reference to FIG. 5 , and the imaging method of this embodiment is specifically implemented by the following steps:

步骤一、选取488nm、532nm、633nm以及785nm波长的激光器,以单模光纤作为耦合媒介,组合搭建形成多通路激发光模块;Step 1: Select lasers with wavelengths of 488nm, 532nm, 633nm and 785nm, use single-mode fiber as the coupling medium, and combine to form a multi-channel excitation light module;

步骤二、选取特定的拉曼探针分子(荧光探针分子),将其与抗体结合,对样品进行特异性标记;Step 2: Select a specific Raman probe molecule (fluorescent probe molecule), combine it with an antibody, and specifically label the sample;

步骤三、开启激发光模块,以倒置荧光显微镜为平台放置待测样品,并利用激发光路产生的结构光条纹对样品进行探针信号的激发;值得注意的是,为了实现各向同性的超分辨成像,需采用三个不同方向的正弦条纹,对样品进行激发照明。由于激发光源模块包含四种不同激发波长,因此在光路中加入能够对波长进行分选的声光调制器,根据具体采用的探针对入射波长进行选通;Step 3: Turn on the excitation light module, place the sample to be tested with the inverted fluorescence microscope as a platform, and use the structured light stripes generated by the excitation light path to excite the probe signal of the sample; it is worth noting that in order to achieve isotropic super-resolution For imaging, three sinusoidal fringes in different directions are used to excite and illuminate the sample. Since the excitation light source module contains four different excitation wavelengths, an acousto-optic modulator capable of sorting wavelengths is added to the optical path, and the incident wavelength is gated according to the specific probe used;

步骤四、被激发出来探针的信号将到达拉曼分光成像模块,通过成像模块中的滤光片转轮实现信号的特异性分选,而后成像于CCD;Step 4. The signal of the excited probe will reach the Raman spectroscopic imaging module, and the specific sorting of the signal will be realized by the filter wheel in the imaging module, and then imaged on the CCD;

步骤五、对采集的信号进行数据处理,重构获得具有二倍衍射极限的超分辨成像。Step 5: Perform data processing on the collected signals, and reconstruct to obtain super-resolution imaging with twice the diffraction limit.

本实施方式中,用于特异性标记的探针为拉曼探针或荧光探针。被测样品包括活细胞、细胞膜、人工磷脂膜、能内吞或转运单个分子及颗粒的体系。所述抗体可以为表皮生长因子受体(EGFR)抗体或葡萄糖转体蛋白(GLUT1)抗体等。In this embodiment, the probes used for specific labeling are Raman probes or fluorescent probes. Test samples include living cells, cell membranes, artificial phospholipid membranes, and systems capable of endocytosing or transporting single molecules and particles. The antibody can be epidermal growth factor receptor (EGFR) antibody or glucose transfectin (GLUT1) antibody, and the like.

本实施方式中将多通路结构光照明超分辨显微成像方法与特异性拉曼成像技术相结合,能够在复杂体系下,获取不同拉曼探针标记下的多个目标观测物的特异性超分辨成像信息,可用于内吞/转运单个分子及颗粒体系、病毒进入细胞机理、活细胞内分子的动态过程等研究方向。In this embodiment, the multi-channel structured light illumination super-resolution microscopy imaging method is combined with the specific Raman imaging technology, which can obtain the specific super-resolution imaging of multiple target observations marked with different Raman probes in a complex system. Resolved imaging information can be used in research directions such as endocytosis/transport of single molecules and particle systems, the mechanism of virus entry into cells, and the dynamic process of molecules in living cells.

Claims (8)

1. multi-path Structured Illumination Raman super-resolution micro imaging method, it is characterized in that;Including imaging system, the imaging system System includes excitation module, Structured Illumination module and raman spectroscopy image-forming module;This method is realized by following steps:
Step 1: choosing specific Raman microprobe molecule, by the Raman microprobe molecule in conjunction with antibody, sample is carried out Specific marker;
Step 2: excitation module is opened, and using inverted fluorescence microscope as platform, the striation of the Structured Illumination module outgoing Line excites sample;
Step 3: the signal for the probe that is excited out realizes the specificity sorting of signal by raman spectroscopy image-forming module, then It is imaged at CCD, reconstruct obtains the super-resolution imaging with two times of diffraction limits.
2. multi-path Structured Illumination Raman super-resolution micro imaging method according to claim 1, it is characterised in that: institute State the laser that excitation module includes coupler (1), single mode optical fiber (2) and different wave length;
The Structured Illumination module includes collimator (3), acousto-optic modulator (4), expands microscope group (5), half-wave plate (6), PBS point Beam device (7), ferroelectric liquid crystals (8), first group of lens (9), Pockers cell (10), reflecting mirror (11), second group of lens (12), first Converging lenses (13), mask plate (14), collimating mirror (15) and the second converging lenses (16);
The raman spectroscopy image-forming module includes Guan Jing (17), the electronic runner (18) and CCD for being loaded with narrow band filter slice;
The laser of the laser emitting of the different wave length converges at coupler (1) through the reflection of corresponding dichroscope respectively, passes through Coupler (1) is coupled to single mode optical fiber (2);
The divergent beams of single mode optical fiber (2) the coupling outgoing are collimated by collimator (3);It is selected again by acousto-optic modulator (4) The laser of different wave length expands beam size by expanding microscope group (5);Then pass through half-wave plate (6) for light polarization It is adjusted to be reflexed to the light beam in the direction S on ferroelectric liquid crystals (8), by PBS beam splitter (7) by ferroelectric liquid crystals picture behind the direction S Light beam is diffracted into multi beam outgoing by the load of element;Multi-beam is successively through first group of lens (9), Pockers cell (10), reflecting mirror (11) and after second group of lens (12), mask plate (14) is reached by the first converging lenses (13), pass through ± the 1 of mask plate (14) Grade light beam by collimating mirror (15) collimation and the second converging lenses (16) focusing, into inverted fluorescence microscope, finally in object The focal plane of mirror realizes that striations excites sample;
The Raman signal of sample excitation is imaged after filtering by Guan Jing (17) and by narrow band filter in CCD camera.
3. multi-path Structured Illumination Raman super-resolution micro imaging method according to claim 1, which is characterized in that use In specific marker probe be Raman microprobe or fluorescence probe.
4. multi-path Structured Illumination Raman super-resolution micro imaging method according to claim 1, which is characterized in that quilt Sample includes the system of living cells, cell membrane, artificial phospholipid's film, energy endocytosis or transhipment individual molecule and particle.
5. multi-path Structured Illumination Raman super-resolution micro imaging method according to claim 1, which is characterized in that institute Stating antibody is that EGF-R ELISA (EGFR) antibody or glucose turn albumen (GLUT1) antibody.
6. multi-path Structured Illumination Raman super-resolution micro imaging method according to claim 2, which is characterized in that swash The laser of different wave length includes outgoing tetra- excitation wavelengths of 488nm, 532nm, 633nm and 785nm in light emitting module.
7. multi-path Structured Illumination Raman super-resolution micro imaging method according to claim 2, which is characterized in that In In raman spectroscopy image-forming module, using the narrow band filter of electronic runner and different central wavelengths with multiple hole locations to difference The peak signal of Raman microprobe carries out sorting imaging.
8. multi-path Structured Illumination Raman super-resolution micro imaging method according to claim 2, which is characterized in that institute It states and is loaded with the hole location that the electronic runner (18) of narrow band filter slice has been provided with, the hole location of the sky is under fluorescence probe label Traditional structure light super-resolution imaging.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11358984B2 (en) 2018-08-27 2022-06-14 Regeneran Pharmaceuticals, Inc. Use of Raman spectroscopy in downstream purification

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102004006391A1 (en) * 2004-02-10 2005-09-01 Universität Leipzig Raman probe for measuring the Raman effect in solid bodies and during semiconductor crystal growth processes has coupling prisms, compound lenses and a narrow band pass filter arranged between the last two compound lenses
US20070002319A1 (en) * 2005-04-29 2007-01-04 Knopp Kevin J Method and apparatus for conducting Raman spectroscopy
TWM515103U (en) * 2015-06-11 2016-01-01 Univ Nat Cheng Kung Variable light source Raman spectroscopy capture apparatus
CN105482803A (en) * 2015-11-26 2016-04-13 东南大学 Fluorescence-SERS dual-mode super-resolution imaging probe and its preparation method and use method
CN108107034A (en) * 2017-12-27 2018-06-01 中国科学院长春应用化学研究所 Raman super-resolution micro imaging system and imaging method based on Structured Illumination
CN108337901A (en) * 2015-12-07 2018-07-27 深圳源光科技有限公司 A kind of biological sensor
CN109407295A (en) * 2018-12-18 2019-03-01 中国科学院深圳先进技术研究院 It is a kind of based on DMD can polychrome excitation structure light microscopic system and polychrome exciting method

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102004006391A1 (en) * 2004-02-10 2005-09-01 Universität Leipzig Raman probe for measuring the Raman effect in solid bodies and during semiconductor crystal growth processes has coupling prisms, compound lenses and a narrow band pass filter arranged between the last two compound lenses
US20070002319A1 (en) * 2005-04-29 2007-01-04 Knopp Kevin J Method and apparatus for conducting Raman spectroscopy
TWM515103U (en) * 2015-06-11 2016-01-01 Univ Nat Cheng Kung Variable light source Raman spectroscopy capture apparatus
CN105482803A (en) * 2015-11-26 2016-04-13 东南大学 Fluorescence-SERS dual-mode super-resolution imaging probe and its preparation method and use method
CN108337901A (en) * 2015-12-07 2018-07-27 深圳源光科技有限公司 A kind of biological sensor
CN108107034A (en) * 2017-12-27 2018-06-01 中国科学院长春应用化学研究所 Raman super-resolution micro imaging system and imaging method based on Structured Illumination
CN109407295A (en) * 2018-12-18 2019-03-01 中国科学院深圳先进技术研究院 It is a kind of based on DMD can polychrome excitation structure light microscopic system and polychrome exciting method

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
普朝光等主编: "《光波光学》", 31 January 2013 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11358984B2 (en) 2018-08-27 2022-06-14 Regeneran Pharmaceuticals, Inc. Use of Raman spectroscopy in downstream purification

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