CN214953038U - Super-resolution microscopic imaging system - Google Patents
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Abstract
The embodiment of the utility model discloses super-resolution microscopic imaging system. The system comprises: the device comprises an excitation light source generating module, an imaging module, a focal plane locking module and a control and data acquisition module; the excitation light source generating module is used for generating an excitation light source; the imaging module is used for receiving an excitation light source, irradiating the excitation light source on a sample of the sample slide to enable a sample field area to generate fluorescence, and collecting the reflected fluorescence through a camera; the focal plane locking module is used for transmitting laser to the imaging module and receiving the laser reflected by the imaging module so as to lock the distance between an objective lens in the imaging module and the sample slide; the control and data acquisition module is used for controlling and adjusting optical elements in the excitation light source generation module, the imaging module and the focal plane locking module, and acquiring fluorescence data obtained by the imaging module to analyze the data. The system realizes the single molecule positioning microscopic technology which is compact, high in automation degree, adjustable and controllable, and improves the precision and the accuracy.
Description
Technical Field
The embodiment of the utility model provides a relate to microscopic imaging technology field, especially relate to a super-resolution microscopic imaging system.
Background
Fluorescence microscopy, by virtue of its good molecular specificity and the ability to image non-invasively, is the most widespread technique used for the visual analysis of biological cells. Due to the diffraction of light, the resolution of the conventional optical microscope cannot always break through the abbe diffraction limit, i.e. half of the wavelength of light, about 250 nm. Most biomolecule and molecular complex structures are less than 100 nm in size, and therefore, researchers have been unable to clearly observe detailed information of biomolecules and cells for a long period of time in the past. In recent years, X-ray crystallography, nuclear magnetic resonance, and cryoelectron microscopy techniques have made it possible to deconstruct biological three-dimensional structures on the order of angstroms, with improvements in hardware and imaging methods. However, because these techniques usually have extremely high requirements for the observation environment, and require complicated pretreatment steps (purification, crystallization, freezing, etc.) for the sample to be tested, and in addition, considering the high equipment cost, the in-situ research of the three-dimensional structure and composition (such as protein complex, three-dimensional genome structure, etc.) of biological macromolecules in cells still remains a huge challenge. With the progress of laser technology, optical field regulation theory and fluorescence labeling method, the super-resolution imaging technology based on optical Microscopy has made great progress in recent years, including structured light Microscopy (SIM), Stimulated Emission Depletion fluorescence Microscopy (STED), Single Molecule Localization Microscopy (SMLM), and the like. These techniques extend the resolution of optical microscopy to the nanoscale by virtue of advances in fluorescence molecular labeling techniques and image reconstruction algorithms. The STED and the SIM modulate the illumination light through an optical method, and inhibit the fluorescence molecules in a diffraction limit area from simultaneously carrying out fluorescence emission by utilizing a saturation mechanism of the fluorescence molecules, so that the size of the Airy spot is reduced, and the purpose of breaking through the diffraction limit is achieved. The SMLM randomly excites a single fluorescent molecule in a diffraction limit area at different times to achieve the purpose of breaking through the diffraction limit. Compared with STED and SIM, SMLM is currently the highest resolution super-resolution microscopy technology, and is currently the most widely used super-resolution technology due to its relatively simple hardware structure.
However, the conventional SMLM is generally implemented by modifying a commercial wide-field microscope, and often has the phenomena of redundant functions and low compactness, and when the SMLM is applied specifically, the problems of difficulty in modification and upgrade, high cost, incapability of meeting requirements and the like exist, and the requirement of acquiring in-situ real-time molecular motion original images in cells cannot be met.
SUMMERY OF THE UTILITY MODEL
The embodiment of the utility model provides a super-resolution microscopic imaging system to the compactedness and the adjustable controllability of improvement system, thereby the demand problem of the real-time molecule activity original image information of normal position in the solution collection cell improves the precision and the rate of accuracy of the micro method of current monomolecular location.
The embodiment of the utility model provides a super-resolution microscopic imaging system, include: the device comprises an excitation light source generating module, an imaging module, a focal plane locking module and a control and data acquisition module; wherein the content of the first and second substances,
the excitation light source generating module is used for generating an excitation light source;
the imaging module is used for receiving the excitation light source, irradiating the excitation light source on a sample of the sample slide to enable a sample field area to generate fluorescence, and collecting the reflected fluorescence through a camera;
the focal plane locking module is used for emitting laser to the imaging module and receiving the laser reflected by the imaging module so as to measure and lock the distance between the objective lens in the imaging module and the sample slide; the imaging module is also used for irradiating the laser emitted by the focal plane locking module on the sample slide;
the control and data acquisition module is used for controlling and adjusting optical elements in the excitation light source generation module, the imaging module and the focal plane locking module, and acquiring fluorescence data obtained by the imaging module to perform data analysis.
Optionally, the imaging module includes a dichroic mirror, a deformable mirror, a first optical path unit, and a second optical path unit; the dichroic mirror is used for dividing the reflected fluorescence into a first path of fluorescence and a second path of fluorescence, the first path of fluorescence is converged to a first channel of the camera through the first light path unit, and the second path of fluorescence is converged to a second channel of the camera through the deformable mirror and the second light path unit in sequence.
Optionally, the imaging module further includes a cylindrical mirror and a first servo motor, where the first servo motor is used to control whether to add the cylindrical mirror into the light path in front of the dichroic mirror.
Optionally, the imaging module further includes a first optical filter, a second servo motor, and a third servo motor; the second servo motor is used for controlling whether the first optical filter is added into the optical path between the dichroic mirror and the first optical path unit, the third servo motor is used for controlling whether the second optical filter is added into the optical path between the dichroic mirror and the deformable reflecting mirror, and the first optical filter and the second optical filter are used for filtering stray light in the optical path.
Optionally, the imaging module further includes a first lens and a fourth servo motor; and the fourth servo motor is used for controlling whether the first lens is added into the light path in front of the camera or not so as to observe the condition of the rear focal plane of the objective lens.
Optionally, the excitation light source generating module includes a first excitation light source generating unit and a second excitation light source generating unit; the first excitation light source generating unit comprises at least one electric reflector and at least two couplers, the electric reflector is used for selecting a target coupler from the couplers to output the excitation light source to the corresponding second excitation light source generating unit, and the second excitation light source generating unit is used for adjusting the received excitation light source and then irradiating the adjusted excitation light source on the imaging module.
Optionally, the first excitation light source generating unit includes a plurality of first lasers with different wavelengths, at least one long-wave pass dichroic mirror, and an acousto-optic tunable filter; and laser emitted by each first laser is converged on the acousto-optic tunable filter through the at least one long-wave-pass dichroic mirror, and the acousto-optic tunable filter is used for controlling the wavelength and the illumination light intensity of the excitation light source and irradiating the excitation light source onto the electric reflector.
Optionally, the second excitation light source generating unit includes a reflecting mirror, and the reflecting mirror is disposed on the linear displacement table and is configured to reflect the adjusted excitation light source to the imaging module, and focus the adjusted excitation light source on different positions of a back focal plane of the objective lens by moving the linear displacement table.
Optionally, the focal plane locking module includes a second laser, a second lens, a D-shaped mirror, and a four-quadrant photodiode; laser emitted by the second laser irradiates the imaging module through the second lens, and the reflected laser is reflected to the four-quadrant photodiode through the D-shaped reflector; the imaging module comprises a z-axis displacement stage for adjusting the distance between the sample slide and the objective lens, and the focal plane locking module further comprises a controller for adjusting or locking the z-axis displacement stage according to the position of the laser irradiation on the four-quadrant photodiode.
Optionally, the control and data acquisition module includes a computer and an electronic control device, the computer is configured to acquire and analyze fluorescence data obtained by the imaging module, and control and adjust optical elements in the excitation light source generation module, the imaging module, and the focal plane locking module through the electronic control device.
The embodiment of the utility model provides a super-resolution microscopic imaging system through realizing the microscopic technique of monomolecular location alone with the modular mode, and the function is with strong points, and the compactness is higher. And some optical elements used in the system are adjustable and controllable, so that the mode state of the system can be conveniently adjusted, the experimental configuration requirement of single-molecule image data is met, the precision and the accuracy of the existing single-molecule positioning microscopy method are improved, an imaging light path is easy to build and test, the reconstruction and the upgrade are easier, and the cost can be reduced. In addition, the distance between the objective lens and the sample slide is measured and locked by arranging the focal plane locking module, so that real-time axial drift correction is realized.
Drawings
Fig. 1 is a schematic structural diagram of a super-resolution micro-imaging system according to an embodiment of the present invention;
fig. 2 is a detailed structural diagram of an excitation light source generating module, an imaging module, and a focal plane locking module according to an embodiment of the present invention.
Detailed Description
The present invention will be described in further detail with reference to the accompanying drawings and examples. It is to be understood that the specific embodiments described herein are merely illustrative of the invention and are not limiting of the invention. It should be further noted that, for the convenience of description, only some of the structures related to the present invention are shown in the drawings, not all of the structures. Based on the embodiment of the present invention, all other embodiments obtained by the skilled in the art without creative work all belong to the protection scope of the present invention.
Furthermore, the terms "first," "second," and the like may be used herein to describe various orientations, actions, steps, elements, or the like, but the orientations, actions, steps, or elements are not limited by these terms. These terms are only used to distinguish one direction, action, step or element from another direction, action, step or element. The terms "first", "second", etc. are not to be construed as indicating or implying relative importance or implicitly indicating the number of technical features indicated. Thus, a feature defined as "first" or "second" may explicitly or implicitly include one or more of that feature.
Example one
Fig. 1 is a schematic structural diagram of a super-resolution micro-imaging system according to an embodiment of the present invention. As shown in fig. 1, the system includes: the device comprises an excitation light source generating module a, an imaging module b, a focal plane locking module c and a control and data acquisition module d; the excitation light source generating module a is used for generating an excitation light source; the imaging module b is used for receiving an excitation light source, irradiating the excitation light source on a sample of the sample slide to enable a sample field area to generate fluorescence, and collecting the reflected fluorescence through a camera; the focal plane locking module c is used for emitting laser to the imaging module b and receiving the laser reflected by the imaging module b so as to measure and lock the distance between the objective lens in the imaging module b and the sample slide; the imaging module b is also used for irradiating the laser emitted by the focal plane locking module c on the sample slide; the control and data acquisition module d is used for controlling and adjusting optical elements in the excitation light source generation module a, the imaging module b and the focal plane locking module c, and acquiring fluorescence data obtained by the imaging module b for data analysis.
Specifically, the excitation light source generation module a is configured to provide an excitation light source for the imaging module b, and the imaging module b includes an objective lens and a sample slide, where the objective lens may be a large-numerical-aperture microscope objective lens, and is configured to perform a main amplification effect on a sample image. When the excitation light source generation module a generates an excitation light source and is received by the imaging module b, the imaging module b can reflect the excitation light source to the back focal plane of the objective lens and irradiate the sample on the sample slide through the objective lens, and under the action of the excitation light source, the sample field area generates fluorescence, and the generated fluorescence can be collected by the objective lens. The imaging module b further comprises a camera, and the fluorescence collected by the objective lens can finally reach the camera for imaging through a series of light paths after exiting. Wherein the camera may be an sCMOS camera with the conventional function of setting the exposure time and recording the frame and then storing the image to a computer or the like.
Focal plane locking module c also can provide a bunch of laser to imaging module b, imaging module b can be with this bunch of laser reflection to objective back focal plane on, and from objective outgoing, can pass through a series of light paths and finally return focal plane locking module c after the lower surface of sample slide takes place to reflect, focal plane locking module c then can be according to the state measurement of the light beam that returns and obtain the distance between objective lens and the sample slide, then can adjust the distance between objective lens and the sample slide through a feedback system, and realize focal plane locking according to the parameter that sets for in advance.
The control and data acquisition module d can be connected with the excitation light source generation module a, the imaging module b and the focal plane locking module c, and can control and adjust some adjustable and controllable optical elements, such as a laser, a displacement table, a servo motor, an acousto-optic tunable filter, an electric reflector, a deformable reflector and the like, so as to adjust the light path to a required state. Meanwhile, the control and data acquisition module d can also acquire fluorescence data by being connected with a camera in the imaging module b, and can perform synchronous data analysis on the acquired fluorescence data.
Alternatively, as shown in fig. 2, the imaging module b includes a dichroic mirror 45, a deformable mirror 51, a first optical path unit, and a second optical path unit; the dichroic mirror 45 is configured to divide the reflected fluorescence 100 into a first path of fluorescence 101 and a second path of fluorescence 102, where the first path of fluorescence 101 is converged to a first channel (not shown) of the camera 56 through a first optical path unit, and the second path of fluorescence 102 is converged to a second channel (not shown) of the camera 56 through the deformable mirror 51 and a second optical path unit in sequence. Specifically, the dichroic mirror 45 is also called as a dichroic mirror, and almost completely transmits light of a certain wavelength and almost completely reflects light of other wavelengths, and when fluorescence is incident at 45 degrees or a large angle, a specific spectrum can be separated and the light path direction of a part of the spectrum can be changed, so that the structure of the device can be effectively reduced, and a multifunctional light path can be realized, thereby enabling the system to be compact. In this embodiment, the reflected fluorescence 100 may strike the dichroic mirror 45 at an incident angle of 45 degrees, and then the fluorescence is divided into two paths, that is, a first path of fluorescence 101 and a second path of fluorescence 102, the first path of fluorescence 101 is directly converged to the camera 56 through the first optical path unit, the second path of fluorescence 102 is converged to the camera 56 through the deformable mirror 51 and the second optical path unit in sequence, and the camera 56 may simultaneously collect the fluorescence of the two paths. Optionally, the incident angle of the fluorescence incident to the deformable mirror 51 is 15 degrees, and aberration correction for imaging of a thick sample can be realized by adjusting the deformable mirror 51, so that richer cellular molecular content information is mined. Optionally, the first light path unit may include a mirror 49, a mirror 48, a lens 53, and a right-angle prism mirror 54 in sequence, so as to focus the first path of fluorescent light 101 to the first channel of the camera 56, the second light path unit may include a mirror 50, a lens 52, and a right-angle prism mirror 54 in sequence, so as to focus the second path of fluorescent light 102 to the second channel of the camera 56, and the first light path unit and the second light path unit may share the right-angle prism mirror 54, so as to make the system more compact.
Optionally, as shown in fig. 2, the imaging module b further includes a cylindrical mirror 42 and a first servo motor, where the first servo motor is used to control whether to add the cylindrical mirror 42 to the optical path in front of the dichroic mirror 45. Specifically, the movement of the cylindrical mirror 42 can be controlled by controlling the first servo motor to move through the control and data acquisition module d, as shown in fig. 2, when the cylindrical mirror 42 is not added to the light path in front of the dichroic mirror 45, the cylindrical mirror 42 can be controlled to move downward to a specified position to add the light path in front of the dichroic mirror 45 when needed. By controlling whether the cylindrical mirror 42 is added, two-dimensional imaging or three-dimensional imaging can be selected. Wherein the focal length of the cylindrical mirror 42 can be set to 1 meter. Optionally, the imaging module b further includes a third optical path unit in front of the dichroic mirror 45, and may form a main optical path of the imaging module b together with the dichroic mirror 45, the deformable mirror 51, the first optical path unit, and the second optical path unit, where the third optical path unit may sequentially include a multicolor optical filter 40, a sleeve lens 41, a diaphragm 43, and a lens 44, so as to adjust the fluorescence reflected by the sample slide 37, and particularly optimize the placement position of each optical element, so that the system is more compact, specifically, the focal length of the sleeve lens 41 may be set to 180 mm, the focal length of the lens 44 is 125 mm, and the focal lengths of the lens 52 and the lens 53 are 75 mm. Accordingly, the first servomotor can control whether or not the cylindrical lens 42 is added to the optical path between the sleeve lens 41 and the stop 43.
Optionally, as shown in fig. 2, the imaging module b further includes a first optical filter 46, a second optical filter 47, a second servo motor, and a third servo motor; the second servo motor is used for controlling whether to add the first optical filter 46 into the optical path between the dichroic mirror 45 and the first optical path unit, the third servo motor is used for controlling whether to add the second optical filter 47 into the optical path between the dichroic mirror 45 and the deformable reflecting mirror 51, and the first optical filter 46 and the second optical filter 47 are used for filtering stray light in the optical path. Specifically, the movement of the second servo motor and the third servo motor can be controlled by the control and data acquisition module d, so as to control the movement of the first optical filter 46 and the second optical filter 47. The first optical filter 46 and the second optical filter 47 can cooperate with different dichroic mirrors 45 to help the dual-channel main optical path filter stray light, and then the first optical filter 46, the second optical filter 47 and the dichroic mirrors 45 in different wavelength bands can be selected according to actual needs.
Optionally, as shown in fig. 2, the imaging module b further includes a first lens 55 and a fourth servo motor; the fourth servo motor is used to control whether the first lens 55 is added to the optical path before the camera 56 to observe the condition of the objective lens back focal plane 34. Specifically, the fourth servo motor may be controlled to move by the control and data acquisition module d, so as to control the movement of the first lens 55. By adding a first lens 55 in the light path before the camera 56, it is possible to observe the back focal plane 34 of the objective lens on the camera 56.
Optionally, as shown in fig. 2, in the imaging module b, a low-pass dichroic mirror 39 may be added in the light path before the main light path, so that the fluorescence reflected back from the sample slide 37 may be incident into the main light path through the low-pass dichroic mirror 39, and the laser reflected back from the sample slide 37 is reflected to the focal plane locking module c through the low-pass dichroic mirror 39, so as to implement light paths with different functions, and further make the system compact. The fluorescence and/or laser light reflected back from the sample slide 37 can be reflected again to the dichroic mirror 39, in particular by the mirror 38, to optimize the structure of the imaging module b. A dichroic mirror 33 may be added to the optical path in front of the reflecting mirror 38, so that the excitation light source provided by the excitation light source generating module a is reflected to the objective lens back focal plane 34 through the dichroic mirror 33, and the fluorescence reflected by the sample slide 37 is incident to the reflecting mirror 38 through the dichroic mirror 33, which may further make the system compact.
The specific light beam propagation process may be that the excitation light source is reflected to the objective back focal plane 34 by the dichroic mirror 33, and is irradiated on the sample slide 37 by the objective 36, and meanwhile, the field of view region selection may be performed by an xy-axis electric displacement stage where the sample slide 37 is located, so that fluorescence is generated in the sample field of view region and is collected by the objective 36, and the emergent fluorescence 110 passes through the dichroic mirror 33, passes through the reflecting mirror 38, passes through the low-pass dichroic mirror 39, and enters the main light path of the imaging module b. In the main light path, the fluorescence vertically passes through the multicolor filter 40, the sleeve lens 41, the diaphragm 43 and the lens 44 in sequence, and strikes the dichroic mirror 45 at an incident angle of 45 degrees, the fluorescence backwards is divided into two paths, one path vertically passes through the lens 53 after passing through the reflecting mirror 49 and the reflecting mirror 48, and finally converges on the camera 56 at an exit angle of 45 degrees under the action of the right-angle prism reflecting mirror 54, the other path vertically passes through the lens 52 after passing through the deformable reflecting mirror 51 and the reflecting mirror 50, and converges on the camera 56 at an exit angle of 45 degrees under the action of the right-angle prism reflecting mirror 54, and finally the fluorescence of the two paths is simultaneously collected by the camera 56.
Alternatively, as shown in fig. 2, the excitation light source generation module a includes a first excitation light source generation unit a1 and a second excitation light source generation unit a 2; the first excitation light source generation unit a1 includes at least one motorized mirror (for example, fig. 2 includes two motorized mirrors 20 and 21) and at least two couplers (for example, fig. 2 includes three couplers 22, 23, and 24), the motorized mirrors are used to select a target coupler from the couplers (for example, fig. 2 may select the coupler 24 as the target coupler) and output an excitation light source to the corresponding second excitation light source generation unit a2, and the second excitation light source generation unit a2 is used to adjust the excitation light source received and irradiate the adjusted excitation light source onto the imaging module b. Specifically, the first excitation light source generation unit a1 may generate an excitation light source by a laser, and after the excitation light source is generated, the excitation light source may be incident on the electric mirror 20 to be reflected and irradiated on the coupler 23 via the mirror 17 and the mirror 16, or may be incident on the electric mirror 21 to be reflected and irradiated on the coupler 24 via the mirror 19 and the mirror 18 after passing through the electric mirror 20 and the electric mirror 21, or may be directly irradiated on the coupler 22 after passing through the electric mirror 20 and the electric mirror 21 in sequence, thereby implementing the selection process of the target coupler. The transmission or reflection can be realized by controlling the electric reflector through the control and data acquisition module d, and the purpose of providing excitation light sources for different equipment can be achieved by arranging the electric reflector.
Alternatively, as shown in fig. 2, the first excitation light source generation unit a1 includes a plurality of first lasers (for example, four of the first laser 1, the first laser 2, the first laser 3, and the first laser 4 are included in fig. 2), at least one long-wavelength pass dichroic mirror (for example, three of the long-wavelength pass dichroic mirror 10, the long-wavelength pass dichroic mirror 11, and the long-wavelength pass dichroic mirror 12 are included in fig. 2), and an acousto-optic tunable filter 13, which have different wavelengths; the laser emitted by each first laser is converged on the acousto-optic tunable filter 13 through at least one long-wave-pass dichroic mirror, and the acousto-optic tunable filter 13 is used for controlling the wavelength and the illumination intensity of an excitation light source and irradiating the excitation light source onto the electric reflector. Specifically, as shown in fig. 2, the laser light emitted from the first laser 1 sequentially passes through the reflecting mirror 5, the reflecting mirror 9, the long-wave-pass dichroic mirror 10, the long-wave-pass dichroic mirror 11, and the long-wave-pass dichroic mirror 12, the laser light emitted from the first laser 2 sequentially passes through the reflecting mirror 6, the long-wave-pass dichroic mirror 10, the long-wave-pass dichroic mirror 11, and the long-wave-pass dichroic mirror 12, the laser light emitted from the first laser 3 sequentially passes through the reflecting mirror 7, the long-wave-pass dichroic mirror 11, and the long-wave-pass dichroic mirror 12, the laser light emitted from the first laser 4 sequentially passes through the reflecting mirror 8 and the long-wave-pass dichroic mirror 12, so that the laser light emitted from the four first lasers can finally converge through the acousto-optic tunable filter 13, and the wavelength of the emergent light and the intensity of the emergent light can be modulated through the acousto-optic tunable filter 13, so as to control the wavelength and the intensity of the excitation light source, to enable the capability of polychromatic fluorescence imaging. The four first lasers can be lasers with wavelengths of 638 nanometers, 561 nanometers, 488 nanometers and 405 nanometers. After modulation of the excitation light source is completed, the excitation light source can be irradiated onto the motorized mirror through the mirror 14 and the mirror 15 for an optimized structure.
Alternatively, as shown in fig. 2, the second excitation light source generation unit a2 includes a mirror (for example, two mirrors 31 and 32 are included in fig. 2), and the mirror is disposed on the linear displacement stage and is used for reflecting the adjusted excitation light source onto the imaging module b and focusing the adjusted excitation light source on different positions of the objective lens back focal plane 34 by moving the linear displacement stage. Specifically, after the target coupler is determined, the generated excitation light source may be coupled into the single-mode polarization maintaining fiber 25, and the excitation light source may be output to the second excitation light source generating unit a2 corresponding to the target coupler through the single-mode polarization maintaining fiber 25, as shown in fig. 2, where the second excitation light source generating unit a2 includes a two-dimensionally translatable optical fiber holder 26, and then the single-mode polarization maintaining fiber 25 may be attached to the optical fiber holder 26 to receive the excitation light source. After entering the second excitation light source generation unit a2, the excitation light source can pass through the lens 27, the filter 28, the diaphragm 29 and the lens 30 in the cage structure in sequence, and finally is focused on the objective lens back focal plane 34 in the imaging module b through the reflecting mirror 31 and the reflecting mirror 32, and the size of the illumination field can be changed by adjusting the diaphragm 29. The reflecting mirror can be arranged on the linear displacement table, and the excitation light source can be focused on different positions of the back focal plane 34 of the objective lens by moving the linear displacement table up and down, so that different illumination modes can be realized.
Optionally, the focal plane locking module c includes a second laser 57, a second lens 60, a D-shaped mirror 61 and a four-quadrant photodiode 62; laser emitted by the second laser 57 is irradiated onto the imaging module b through the second lens 60, and the reflected laser is reflected onto the four-quadrant photodiode 62 through the D-shaped reflector 61; the imaging module b comprises a z-axis displacement stage 35, the z-axis displacement stage 35 is used for adjusting the distance between the sample slide 37 and the lens of the objective lens 36, and the focal plane locking module c further comprises a controller, and the controller is used for adjusting or locking the z-axis displacement stage 35 according to the position of the laser irradiation on the four-quadrant photodiode 62. Specifically, the second lens 60 may be mounted on a translation stage which is movable up and down, and the second laser 57 emits laser light which is irradiated onto the imaging module b via the second lens 60, and by moving the translation stage, the laser light may be focused on the objective lens back focal plane 34, and then the laser light may be emitted from the objective lens 36, reflected on the lower surface of the sample slide 37, and then reflected back to the D-shaped mirror 61, and finally reflected to the four-quadrant photodiode 62 via the D-shaped mirror 61. The z-axis displacement stage 35 can be arranged on the objective lens 36, the distance between the sample slide 37 and the lens of the objective lens 36 can be changed by moving the z-axis displacement stage 35 up and down, and the distance can be changed by changing the position of the folded laser on the four-quadrant photodiode 62, so that the distance between the sample slide 37 and the lens of the objective lens 36 can be measured according to the position of the laser on the four-quadrant photodiode 62. The controller in the focal plane locking module c can form a feedback system with the z-axis displacement table 35, and the distance between the sample slide 37 and the lens of the objective lens 36 can be locked according to preset parameters by matching with the linear displacement table arranged below the four-quadrant photodiode 62, so that real-time axial drift correction is realized. Wherein the second laser 57 may be a laser having a wavelength of 785 nanometers. In addition, in order to optimize the structure of the focal plane locking module c, a mirror 58 and a mirror 59 may be sequentially added to the optical path between the second laser 57 and the second lens 60.
Optionally, the control and data acquisition module d includes a computer and an electronic control device, the computer is used for acquiring and analyzing the fluorescence data obtained by the imaging module b, and controlling and adjusting the optical elements in the excitation light source generation module a, the imaging module b and the focal plane locking module c through the electronic control device. Specifically, the computer may communicate with the microscope apparatus, which includes various optical elements in the excitation light source generation module a, the imaging module b, and the focal plane locking module c, directly or through an electronic control apparatus. At the same time, the electronic control device can also perform different functions, such as monitoring parameters or triggering devices, etc., independently of the computer. On one hand, the computer can be connected with the camera 56 in the imaging module b to collect fluorescence data (cell sample image) and can perform synchronous data analysis, and the data obtained by analysis can be stored on the server, so that a user can perform real-time data retrieval in the server, and the collected original data can be stored on the server after being automatically compressed due to large data volume. On the other hand, the computer can be connected to the electronic control device to control and adjust some of the adjustable and controllable optical elements in the microscope device via the electronic control device. The electronic control device can select a Field Programmable Gate Array (FPGA) as a core controller, and can control the servo motor, the displacement table, the acousto-optic tunable filter, the electric reflector, the deformable reflector, the laser and other optical elements, wherein the displacement table can be controlled by a control handle, and the deformable reflector can be directly communicated with a computer through a USB interface. Specifically, the electronic control device can receive signals from a four-quadrant photodiode or other various sensors through analog input, and control linkage triggering between the laser and the camera, movement of the servo motor and the electric reflector, modulation of the acousto-optic tunable filter and the like through TTL/PWM and other signal output. Most optical elements in the system are controllable and adjustable, so that the mode state of the microscope can be adjusted conveniently, the experimental configuration requirements of single-molecule image data are met, and meanwhile, an imaging light path is easy to build and test. The system can also optimize the optical path by optical design software Zemax in advance, and design the mechanical structure of the corresponding optical element supporting adjusting frame on the basis of the optimized optical path so as to finally achieve the purpose of adjustable, controllable and compact design. The system can also appropriately modify the size, the structure and the like of the elements according to the specific imaging data acquisition requirements, can be adapted to lasers, cameras, objective lenses, displacement tables, various optical elements and the like of different types, and has strong flexibility.
In addition, a software control interface Micro-Manager hosted by a computer can be provided for a user to supervise and control various processes, and related microscope parameters can be configured by the user and can be realized by controlling the functions of various modules, wherein the microscope parameters can comprise laser intensity and trigger mode, positions of an optical filter, a lens, a cylindrical mirror and a reflecting mirror, positions of a lens displacement table, an image acquisition mode and the like, so that focal plane locking, focus stabilization adjustment, displacement table positioning and the like can be realized according to preset parameters. The computer can also automatically control the microscope device without user involvement, and particularly, the system can automatically perform experiments according to specific designs through continuous feedback and synchronization between the computer and the electronic control device.
The embodiment of the utility model provides a super-resolution microscopic imaging system through realizing the microscopic technique of monomolecular location alone with the modular mode, and the function is with strong points, and the compactness is higher. And some optical elements used in the system are adjustable and controllable, so that the mode state of the system can be conveniently adjusted, the experimental configuration requirement of single-molecule image data is met, the precision and the accuracy of the existing single-molecule positioning microscopy method are improved, an imaging light path is easy to build and test, the reconstruction and the upgrade are easier, and the cost can be reduced. In addition, the distance between the objective lens and the sample slide is measured and locked by arranging the focal plane locking module, so that real-time axial drift correction is realized.
It should be noted that the foregoing is only a preferred embodiment of the present invention and the technical principles applied. It will be understood by those skilled in the art that the present invention is not limited to the particular embodiments described herein, but is capable of various obvious changes, rearrangements and substitutions as will now become apparent to those skilled in the art without departing from the scope of the invention. Therefore, although the present invention has been described in greater detail with reference to the above embodiments, the present invention is not limited to the above embodiments, and may include other equivalent embodiments without departing from the scope of the present invention.
Claims (10)
1. A super-resolution microscopy imaging system, comprising: the device comprises an excitation light source generating module, an imaging module, a focal plane locking module and a control and data acquisition module; wherein the content of the first and second substances,
the excitation light source generating module is used for generating an excitation light source;
the imaging module is used for receiving the excitation light source, irradiating the excitation light source on a sample of the sample slide to enable a sample field area to generate fluorescence, and collecting the reflected fluorescence through a camera;
the focal plane locking module is used for emitting laser to the imaging module and receiving the laser reflected by the imaging module so as to measure and lock the distance between the objective lens in the imaging module and the sample slide; the imaging module is also used for irradiating the laser emitted by the focal plane locking module on the sample slide;
the control and data acquisition module is used for controlling and adjusting optical elements in the excitation light source generation module, the imaging module and the focal plane locking module, and acquiring fluorescence data obtained by the imaging module to perform data analysis.
2. The super-resolution microscopic imaging system according to claim 1, wherein the imaging module comprises a dichroic mirror, a deformable mirror, a first optical path unit, and a second optical path unit; the dichroic mirror is used for dividing the reflected fluorescence into a first path of fluorescence and a second path of fluorescence, the first path of fluorescence is converged to a first channel of the camera through the first light path unit, and the second path of fluorescence is converged to a second channel of the camera through the deformable mirror and the second light path unit in sequence.
3. The super-resolution microscopy imaging system according to claim 2, wherein the imaging module further comprises a cylindrical mirror and a first servo motor, wherein the first servo motor is used for controlling whether the cylindrical mirror is added to the light path in front of the dichroic mirror.
4. The super-resolution microscopic imaging system according to claim 2, wherein the imaging module further comprises a first optical filter, a second servo motor and a third servo motor; the second servo motor is used for controlling whether the first optical filter is added into the optical path between the dichroic mirror and the first optical path unit, the third servo motor is used for controlling whether the second optical filter is added into the optical path between the dichroic mirror and the deformable reflecting mirror, and the first optical filter and the second optical filter are used for filtering stray light in the optical path.
5. The super resolution microscopic imaging system according to claim 2, wherein the imaging module further comprises a first lens and a fourth servo motor; and the fourth servo motor is used for controlling whether the first lens is added into the light path in front of the camera or not so as to observe the condition of the rear focal plane of the objective lens.
6. The super-resolution microscopic imaging system according to claim 1, wherein the excitation light source generation module comprises a first excitation light source generation unit and a second excitation light source generation unit; the first excitation light source generating unit comprises at least one electric reflector and at least two couplers, the electric reflector is used for selecting a target coupler from the couplers to output the excitation light source to the corresponding second excitation light source generating unit, and the second excitation light source generating unit is used for adjusting the received excitation light source and then irradiating the adjusted excitation light source on the imaging module.
7. The super-resolution microscopic imaging system according to claim 6, wherein the first excitation light source generating unit comprises a plurality of first lasers of different wavelengths, at least one long-wave pass dichroic mirror, and an acousto-optic tunable filter; and laser emitted by each first laser is converged on the acousto-optic tunable filter through the at least one long-wave-pass dichroic mirror, and the acousto-optic tunable filter is used for controlling the wavelength and the illumination light intensity of the excitation light source and irradiating the excitation light source onto the electric reflector.
8. The super-resolution microscopic imaging system according to claim 6, wherein the second excitation light source generating unit comprises a reflecting mirror disposed on a linear displacement stage for reflecting the adjusted excitation light source to the imaging module and focusing the adjusted excitation light source on different positions of a back focal plane of an objective lens by moving the linear displacement stage.
9. The super-resolution microscopic imaging system according to claim 1, wherein the focal plane locking module comprises a second laser, a second lens, a D-shaped mirror, and a four-quadrant photodiode; laser emitted by the second laser irradiates the imaging module through the second lens, and the reflected laser is reflected to the four-quadrant photodiode through the D-shaped reflector; the imaging module comprises a z-axis displacement stage for adjusting the distance between the sample slide and the objective lens, and the focal plane locking module further comprises a controller for adjusting or locking the z-axis displacement stage according to the position of the laser irradiation on the four-quadrant photodiode.
10. The super-resolution microscopic imaging system according to claim 1, wherein the control and data acquisition module comprises a computer and an electronic control device, the computer is used for acquiring and analyzing the fluorescence data obtained by the imaging module, and the electronic control device is used for controlling and adjusting optical elements in the excitation light source generation module, the imaging module and the focal plane locking module.
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