CN112596256A - Optical coherent imaging system capable of reducing optical path dispersion and imaging method - Google Patents
Optical coherent imaging system capable of reducing optical path dispersion and imaging method Download PDFInfo
- Publication number
- CN112596256A CN112596256A CN202110239421.XA CN202110239421A CN112596256A CN 112596256 A CN112596256 A CN 112596256A CN 202110239421 A CN202110239421 A CN 202110239421A CN 112596256 A CN112596256 A CN 112596256A
- Authority
- CN
- China
- Prior art keywords
- imaging system
- unit
- polarizer
- optical path
- image
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 238000003384 imaging method Methods 0.000 title claims abstract description 83
- 230000003287 optical effect Effects 0.000 title claims abstract description 68
- 230000001427 coherent effect Effects 0.000 title claims abstract description 52
- 239000006185 dispersion Substances 0.000 title claims abstract description 50
- 238000001514 detection method Methods 0.000 claims abstract description 29
- 230000005540 biological transmission Effects 0.000 claims abstract description 23
- 230000010287 polarization Effects 0.000 claims abstract description 14
- 238000004458 analytical method Methods 0.000 claims abstract description 12
- 239000013307 optical fiber Substances 0.000 abstract description 13
- 238000005516 engineering process Methods 0.000 abstract description 6
- 238000000034 method Methods 0.000 abstract description 6
- 238000001356 surgical procedure Methods 0.000 description 11
- 238000012014 optical coherence tomography Methods 0.000 description 4
- 239000000835 fiber Substances 0.000 description 3
- 238000005259 measurement Methods 0.000 description 3
- 230000008569 process Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000002457 bidirectional effect Effects 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000012634 optical imaging Methods 0.000 description 1
- 239000002861 polymer material Substances 0.000 description 1
- 230000002980 postoperative effect Effects 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
- 230000004044 response Effects 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/28—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for polarising
- G02B27/286—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for polarising for controlling or changing the state of polarisation, e.g. transforming one polarisation state into another
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/0025—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical correction, e.g. distorsion, aberration
- G02B27/0031—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical correction, e.g. distorsion, aberration for scanning purposes
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Investigating Or Analysing Materials By Optical Means (AREA)
Abstract
本申请提供的可降光路色散的光学相干成像系统及方法,包括:光源(1)、探测单元(2)、干涉仪(3)、图像束传输单元(4)、参考束传输单元(5)参考束传输单元(5)、数据采集分析单元(6)、控制单元(7)及图像显示单元(8),本申请提供的可降光路色散的光学相干成像系统,采用偏振光成像技术,通过光纤起偏器和偏振耦合器的使用构建协调工作的可降光路色散的光学相干成像系统,不易受到自然环境中杂散光的干扰,降低了整个光路的色散,也大大降低了对光纤色散性能的要求,降低了技术方案实时的难度和成本,提高了成像信号强度和信噪比,提高了检测的精确度和实施手术的安全性。
The optical coherent imaging system and method for reducing optical path dispersion provided by the present application includes: a light source (1), a detection unit (2), an interferometer (3), an image beam transmission unit (4), and a reference beam transmission unit (5) With reference to the beam transmission unit (5), the data acquisition and analysis unit (6), the control unit (7) and the image display unit (8), the optical coherence imaging system with reduced optical path dispersion provided by the present application adopts the polarized light imaging technology, through The use of optical fiber polarizers and polarization couplers to construct a coherent optical coherent imaging system that can reduce optical path dispersion, is not easy to be interfered by stray light in the natural environment, reduces the dispersion of the entire optical path, and greatly reduces the impact on the optical fiber dispersion performance. It reduces the real-time difficulty and cost of the technical solution, improves the imaging signal strength and signal-to-noise ratio, improves the detection accuracy and the safety of the operation.
Description
技术领域technical field
本发明属于医疗器械技术领域,具体涉及一种可降光路色散的光学相干成像系统及成像方法。The invention belongs to the technical field of medical devices, and in particular relates to an optical coherent imaging system and an imaging method capable of reducing optical path dispersion.
背景技术Background technique
光学相干层析技术具有非接触、无辐射、高探测灵敏度、无损伤的特点,光学相干层析技术已经成为眼科手术中测量人眼结构的标准技术。而飞秒激光辅助眼科手术,是利用飞秒激光脉冲,光学相干层析技术高精度检测,计算机精密计算进行轨迹规划,将传统眼科手术的几个关键步骤自动化、智能化实现的一种眼科手术。术前、术中和术后需要精确扫描眼组织的位置及轮廓并成像显示给医生。Optical coherence tomography has the characteristics of non-contact, no radiation, high detection sensitivity, and no damage. Optical coherence tomography has become a standard technology for measuring human eye structure in ophthalmic surgery. Femtosecond laser-assisted ophthalmic surgery is an ophthalmic surgery that uses femtosecond laser pulses, optical coherence tomography technology for high-precision detection, and computer precision calculation for trajectory planning, which automates and intelligently realizes several key steps of traditional ophthalmic surgery. . Preoperative, intraoperative and postoperative need to accurately scan the position and contour of eye tissue and image display to the doctor.
目前的技术方案中使用自然光进行测量,受到环境中杂散光的影响,容易引入成像误差,与高精度测量的目的相悖。当可降光路色散的光学相干成像系统探测时容易发生串扰,易受到自然环境中的杂散光的干扰,大大降低了信号强度和信噪比,降低成像的准确性和手术的安全性。In the current technical solution, natural light is used for measurement, which is affected by stray light in the environment and easily introduces imaging errors, which is contrary to the purpose of high-precision measurement. When an optical coherent imaging system that can reduce optical path dispersion is detected, crosstalk is prone to occur, and it is easily interfered by stray light in the natural environment, which greatly reduces the signal strength and signal-to-noise ratio, and reduces the accuracy of imaging and the safety of surgery.
发明内容SUMMARY OF THE INVENTION
鉴于此,有必要针对现有技术存在的缺陷提供一种可提高信号强度和信噪比,提高成像的准确性和手术的安全性的可降光路色散的光学相干成像系统。In view of this, it is necessary to provide an optical coherence imaging system with reduced optical path dispersion, which can improve the signal strength and signal-to-noise ratio, improve the accuracy of imaging and the safety of surgery, aiming at the defects of the prior art.
为解决上述问题,本发明采用下述技术方案:For solving the above problems, the present invention adopts the following technical solutions:
一种可降光路色散的光学相干成像系统,包括:光源(1)、探测单元(2)、干涉仪(3)、图像束传输单元(4)、参考束传输单元(5)、数据采集分析单元(6)、控制单元(7)及图像显示单元(8);所述的图像束传输单元(4)包括依次连接的第一准直透镜(41)、偏振耦合器(42)、二维振镜扫描单元(43)、二向色镜(44)、第二准直透镜(45)、色散补偿器(46)及聚焦透镜(47),所述参考束传输单元(5)包括第一起偏器(51)、第二起偏器(52)及反射镜(53);其中:An optical coherent imaging system capable of reducing optical path dispersion, comprising: a light source (1), a detection unit (2), an interferometer (3), an image beam transmission unit (4), a reference beam transmission unit (5), data acquisition and analysis a unit (6), a control unit (7) and an image display unit (8); the image beam transmission unit (4) includes a first collimating lens (41), a polarization coupler (42), a two-dimensional A galvanometer scanning unit (43), a dichroic mirror (44), a second collimating lens (45), a dispersion compensator (46) and a focusing lens (47), the reference beam transmission unit (5) includes a first a polarizer (51), a second polarizer (52) and a mirror (53); wherein:
所述光源(1)生成扫描波长束经过所述干涉仪(3)分为图像束和参考束;The light source (1) generates a scanning wavelength beam that is divided into an image beam and a reference beam by the interferometer (3);
所述参考束依次进入所述第一起偏器(51)、所述第二起偏器(52)及所述反射镜(53),所述参考束再依次经所述反射镜(53)、所述第二起偏器(52)及所述第一起偏器(51)返回至所述干涉仪(3);The reference beam enters the first polarizer (51), the second polarizer (52) and the mirror (53) in sequence, and the reference beam then passes through the mirror (53), the second polarizer (52) and the first polarizer (51) are returned to the interferometer (3);
所述图像束依次经所述第一准直透镜(41)、所述偏振耦合器(42)、所述二维振镜扫描单元(43)、所述二向色镜(44)、所述第二准直透镜(45)、所述色散补偿器(46)及所述聚焦透镜(47)聚集于眼睛处,并由所述眼睛处将所述图像束返回至所述干涉仪(3);The image beam sequentially passes through the first collimating lens (41), the polarization coupler (42), the two-dimensional galvanometer scanning unit (43), the dichroic mirror (44), the The second collimating lens (45), the dispersion compensator (46) and the focusing lens (47) are collected at the eye and return the image beam from the eye to the interferometer (3) ;
所述的参考束和所述图像束在所述干涉仪(3)处进行相干产生相干光传输至所述探测单元(2),所述探测单元(2)检测所述相干光并传输至所述的数据采集分析单元(6),生成图像信息传递至所述的图像显示单元(8)显示图像信息;The reference beam and the image beam are coherent at the interferometer (3) to generate coherent light, which is transmitted to the detection unit (2), and the detection unit (2) detects the coherent light and transmits it to the detection unit (2). the data acquisition and analysis unit (6), which generates image information and transmits it to the image display unit (8) to display the image information;
所述的控制单元(7)根据所述的图像显示单元(8)生成的图像信息生成控制信号传递至整个可降光路色散的光学相干成像系统进行实时调整。The control unit (7) generates a control signal according to the image information generated by the image display unit (8) and transmits the control signal to the entire optical coherent imaging system capable of reducing optical path dispersion for real-time adjustment.
在其中一些实施例中,所述的第一起偏器(51)和第二起偏器(52)为偏振片。In some of the embodiments, the first polarizer (51) and the second polarizer (52) are polarizers.
在其中一些实施例中,所述成像系统的成像时间为0.01-0.1 秒。In some of these embodiments, the imaging time of the imaging system is 0.01-0.1 seconds.
在其中一些实施例中,所述成像系统的帧率为 50-100 帧/秒。In some of these embodiments, the imaging system has a frame rate of 50-100 frames per second.
在其中一些实施例中,所述成像系统的成像深度为8mm。In some of these embodiments, the imaging system has an imaging depth of 8 mm.
在其中一些实施例中,所述成像系统的成像分辨率为5μm。In some of these embodiments, the imaging resolution of the imaging system is 5 μm.
另外,本发明还提供了一种所述的可降光路色散的光学相干成像系统的成像方法,包括:In addition, the present invention also provides an imaging method of the optical coherent imaging system with reduced optical path dispersion, including:
所述光源(1)生成扫描波长束经过所述干涉仪(3)分为图像束和参考束;The light source (1) generates a scanning wavelength beam that is divided into an image beam and a reference beam by the interferometer (3);
所述参考束依次进入所述第一起偏器(51)、所述第二起偏器(52)及所述反射镜(53),所述参考束再依次经所述反射镜(53)、所述第二起偏器(52)及所述第一起偏器(51)返回至所述干涉仪(3);The reference beam enters the first polarizer (51), the second polarizer (52) and the mirror (53) in sequence, and the reference beam then passes through the mirror (53), the second polarizer (52) and the first polarizer (51) are returned to the interferometer (3);
所述图像束依次经所述第一准直透镜(41)、所述偏振耦合器(42)、所述二维振镜扫描单元(43)、所述二向色镜(44)、所述第二准直透镜(45)、所述色散补偿器(46)及所述聚焦透镜(47)聚集于眼睛处,并由所述眼睛处将所述图像束返回至所述干涉仪(3);The image beam sequentially passes through the first collimating lens (41), the polarization coupler (42), the two-dimensional galvanometer scanning unit (43), the dichroic mirror (44), the The second collimating lens (45), the dispersion compensator (46) and the focusing lens (47) are collected at the eye and return the image beam from the eye to the interferometer (3) ;
所述的参考束和所述图像束在所述干涉仪(3)处进行相干产生相干光传输至所述探测单元(2),所述探测单元(2)检测所述相干光并传输至所述的数据采集分析单元(6),生成图像信息传递至所述的图像显示单元(8)显示图像信息;The reference beam and the image beam are coherent at the interferometer (3) to generate coherent light, which is transmitted to the detection unit (2), and the detection unit (2) detects the coherent light and transmits it to the detection unit (2). the data acquisition and analysis unit (6), which generates image information and transmits it to the image display unit (8) to display the image information;
所述的控制单元(7)根据所述的图像显示单元(8)生成的图像信息生成控制信号传递至整个可降光路色散的光学相干成像系统进行实时调整。The control unit (7) generates a control signal according to the image information generated by the image display unit (8) and transmits the control signal to the entire optical coherent imaging system capable of reducing optical path dispersion for real-time adjustment.
本申请采用上述技术方案具备下述效果:This application adopts the above-mentioned technical scheme to have the following effects:
相较于现有技术,本申请提供的可降光路色散的光学相干成像系统及方法,包括:光源(1)、探测单元(2)、干涉仪(3)、图像束传输单元(4)、参考束传输单元(5)参考束传输单元(5)、数据采集分析单元(6)、控制单元(7)及图像显示单元(8),本申请提供的可降光路色散的光学相干成像系统,采用偏振光成像技术,通过光纤起偏器和偏振耦合器的使用构建协调工作的可降光路色散的光学相干成像系统,不易受到自然环境中杂散光的干扰,降低了整个光路的色散,也大大降低了对光纤色散性能的要求,降低了技术方案实时的难度和成本,提高了成像信号强度和信噪比,提高了检测的精确度和实施手术的安全性。Compared with the prior art, the optical coherent imaging system and method for reducing optical path dispersion provided by the present application includes: a light source (1), a detection unit (2), an interferometer (3), an image beam transmission unit (4), The reference beam transmission unit (5), the reference beam transmission unit (5), the data acquisition and analysis unit (6), the control unit (7) and the image display unit (8), the optical coherent imaging system with reduced optical path dispersion provided by the present application, Using polarized light imaging technology, through the use of fiber polarizers and polarized couplers, a coherent optical coherent imaging system that can reduce optical path dispersion is constructed. The requirements for optical fiber dispersion performance are reduced, the real-time difficulty and cost of technical solutions are reduced, the imaging signal strength and signal-to-noise ratio are improved, the detection accuracy and the safety of performing operations are improved.
附图说明Description of drawings
为了更清楚地说明本发明实施例的技术方案,下面将对本发明实施例或现有技术描述中所需要使用的附图作简单地介绍,显而易见地,下面所描述的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to illustrate the technical solutions of the embodiments of the present invention more clearly, the following briefly introduces the accompanying drawings that are used in the description of the embodiments of the present invention or the prior art. Obviously, the drawings described below are only for the present invention. In some embodiments, for those of ordinary skill in the art, other drawings can also be obtained according to these drawings without any creative effort.
图1为本发明实施例提供的可降光路色散的光学相干成像系统的结构图。FIG. 1 is a structural diagram of an optical coherent imaging system with reduced optical path dispersion provided by an embodiment of the present invention.
其中: 1为光源、2为探测单元、3为干涉仪、4为图像束传输单元、41为第一准直透镜、42为偏振耦合器、43为二维振镜扫描单元、44为二向色镜、45为第二准直透镜、46为色散补偿器、47为聚焦透镜、5为参考束传输单元、51为第一起偏器、52为第二起偏器、53为反射镜、6为数据采集分析单元、7为控制单元、8为图像显示单元、9为人眼。Wherein: 1 is the light source, 2 is the detection unit, 3 is the interferometer, 4 is the image beam transmission unit, 41 is the first collimating lens, 42 is the polarization coupler, 43 is the two-dimensional galvanometer scanning unit, and 44 is the bidirectional Chromatic mirror, 45 is the second collimating lens, 46 is the dispersion compensator, 47 is the focusing lens, 5 is the reference beam transmission unit, 51 is the first polarizer, 52 is the second polarizer, 53 is the mirror, 6 It is a data acquisition and analysis unit, 7 is a control unit, 8 is an image display unit, and 9 is a human eye.
具体实施方式Detailed ways
下面详细描述本发明的实施例,所述实施例的示例在附图中示出,其中自始至终相同或类似的标号表示相同或类似的元件或具有相同或类似功能的元件。下面通过参考附图描述的实施例是示例性的,旨在用于解释本发明,而不能理解为对本发明的限制。The following describes in detail the embodiments of the present invention, examples of which are illustrated in the accompanying drawings, wherein the same or similar reference numerals refer to the same or similar elements or elements having the same or similar functions throughout. The embodiments described below with reference to the accompanying drawings are exemplary, and are intended to explain the present invention and should not be construed as limiting the present invention.
在本发明的描述中,需要理解的是,术语“上”、“下”、“水平”、“内”、“外”等指示的方位或位置关系为基于附图所示的方位或位置关系,仅是为了便于描述本发明和简化描述,而不是指示或暗示所指的装置或元件必须具有特定的方位、以特定的方位构造和操作,因此不能理解为对本发明的限制。In the description of the present invention, it should be understood that the orientation or positional relationship indicated by the terms "upper", "lower", "horizontal", "inner", "outer", etc. is based on the orientation or positional relationship shown in the accompanying drawings , is only for the convenience of describing the present invention and simplifying the description, rather than indicating or implying that the indicated device or element must have a specific orientation, be constructed and operated in a specific orientation, and therefore should not be construed as a limitation of the present invention.
此外,术语“第一”、“第二”仅用于描述目的,而不能理解为指示或暗示相对重要性或者隐含指明所指示的技术特征的数量。由此,限定有“第一”、“第二”的特征可以明示或者隐含地包括一个或者更多个该特征。在本发明的描述中,“多个”的含义是两个或两个以上,除非另有明确具体的限定。In addition, the terms "first" and "second" are only used for descriptive purposes, and should not be construed as indicating or implying relative importance or implying the number of indicated technical features. Thus, a feature defined as "first" or "second" may expressly or implicitly include one or more of that feature. In the description of the present invention, "plurality" means two or more, unless otherwise expressly and specifically defined.
为了使本发明的目的、技术方案及优点更加清楚明白,以下结合附图及实施例,对本发明进行进一步详细说明。In order to make the objectives, technical solutions and advantages of the present invention clearer, the present invention will be further described in detail below with reference to the accompanying drawings and embodiments.
实施例1Example 1
请参阅图1,为本申请实施例1提供的可降光路色散的光学相干成像系统的结构示意图,包括:光源(1)、探测单元(2)、干涉仪(3)、图像束传输单元(4)、参考束传输单元(5)、数据采集分析单元(6)、控制单元(7)及图像显示单元(8);所述的图像束传输单元(4)包括依次连接的第一准直透镜(41)、偏振耦合器(42)、二维振镜扫描单元(43)、二向色镜(44)、第二准直透镜(45)、色散补偿器(46)及聚焦透镜(47),所述参考束传输单元(5)包括第一起偏器(51)、第二起偏器(52)及反射镜(53)。Please refer to FIG. 1, which is a schematic structural diagram of an optical coherent imaging system with reduced optical path dispersion provided in Embodiment 1 of the application, including: a light source (1), a detection unit (2), an interferometer (3), an image beam transmission unit ( 4), a reference beam transmission unit (5), a data acquisition and analysis unit (6), a control unit (7) and an image display unit (8); the image beam transmission unit (4) includes a first collimator connected in sequence Lens (41), polarization coupler (42), two-dimensional galvanometer scanning unit (43), dichroic mirror (44), second collimating lens (45), dispersion compensator (46) and focusing lens (47) ), the reference beam transmission unit (5) includes a first polarizer (51), a second polarizer (52) and a mirror (53).
在其中一些实施例中,所述光纤起偏单元(10)为二向色性的偏振片。In some of the embodiments, the optical fiber polarizing unit (10) is a dichroic polarizer.
可以理解,偏振片用于从自然光中获得偏振光,偏振光的振动方向与偏振片的偏振化方向一致。使用偏振光成像不易受到环境中杂散光的影响,不易引入误差,大大提高了测量的信号强度和信噪比,提高了成像系统的精确度。It can be understood that the polarizer is used to obtain polarized light from natural light, and the vibration direction of the polarized light is consistent with the polarization direction of the polarizer. Using polarized light imaging is not easy to be affected by stray light in the environment, and it is not easy to introduce errors, which greatly improves the measured signal strength and signal-to-noise ratio, and improves the accuracy of the imaging system.
本申请提供的可降光路色散的光学相干成像系统,其工作方式如下:The optical coherent imaging system with reduced optical path dispersion provided by this application works as follows:
所述光源(1)生成扫描波长束经过所述干涉仪(3)分为图像束和参考束;The light source (1) generates a scanning wavelength beam that is divided into an image beam and a reference beam by the interferometer (3);
所述参考束通过所述光纤传输线路(9)依次进入所述第一起偏器(51)、所述第二起偏器(52)及所述反射镜(53),所述参考束再依次经所述反射镜(53)、所述第二起偏器(52)及所述第一起偏器(51)返回至所述干涉仪(3)。The reference beam enters the first polarizer (51), the second polarizer (52) and the reflector (53) in sequence through the optical fiber transmission line (9), and the reference beam then enters in sequence Return to the interferometer (3) via the mirror (53), the second polarizer (52) and the first polarizer (51).
在其中一些实施例中,所述的光纤传输线路(9)为单模光纤,模场直径为6.2μm。In some of the embodiments, the optical fiber transmission line (9) is a single-mode optical fiber, and the mode field diameter is 6.2 μm.
所述单模光纤材质为石英、玻璃或高分子聚合材料找那个的一种。The material of the single-mode optical fiber is one of quartz, glass or polymer materials.
可以理解的是,单模光纤中心芯径很小,本发明采用的是直径为6.2μm,它只能传一种模式的光纤。因此,其模间色散很小,能把光以很宽的频带传输很长距离,而且信号畸变很小,提高了整个光学成像系统的成像精确度。It can be understood that the central core diameter of the single-mode optical fiber is very small, and the present invention adopts an optical fiber with a diameter of 6.2 μm, which can only transmit one mode. Therefore, its intermodal dispersion is very small, light can be transmitted for a long distance with a wide frequency band, and the signal distortion is small, which improves the imaging accuracy of the entire optical imaging system.
所述图像束依次经所述第一准直透镜(41)第一准直透镜(41)、所述偏振耦合器(42)、所述二维振镜扫描单元(43)、所述二向色镜(44)、所述第二准直透镜(45)、所述色散补偿器(46)及所述聚焦透镜(47)聚集于眼睛处,并由所述眼睛处将所述图像束返回至所述干涉仪(3)。The image beam sequentially passes through the first collimating lens (41), the first collimating lens (41), the polarization coupler (42), the two-dimensional galvanometer scanning unit (43), the two-way A chromatic mirror (44), the second collimating lens (45), the dispersion compensator (46) and the focusing lens (47) are collected at the eye, and the image beam is returned from the eye to the interferometer (3).
可以理解的是,采用的偏振耦合器(42)是的自然光改变为偏振光,偏振光的振动方向与偏振片的偏振化方向一致,使用偏振光成像不易受到环境中杂散光的影响,不易引入误差,大大提高了测量的信号强度和信噪比,提高了成像系统的精确度。It can be understood that the polarization coupler (42) used is to change the natural light into polarized light, and the vibration direction of the polarized light is consistent with the polarization direction of the polarizer, and imaging using polarized light is not easily affected by stray light in the environment, and is not easy to introduce. The error greatly improves the measured signal strength and signal-to-noise ratio, and improves the accuracy of the imaging system.
可以理解的是,本发明采用了二维振镜扫描单元(43),振镜的偏转速度极快因而整个扫描速度大大提高,导致成像速度快,成像时间短,意味着可以生成可以提供关于眼科手术进程的及时且因此有用的反馈给医生的图像使得医生可以响应于反馈修改手术过程,可以在进行人眼结构成像过程中可实时观察。在进行飞秒激光辅助眼科手术中,医生可以实时观察患者手术进程,同时两种光学相干层析测量系统协调工作对人眼结构实时成像,能同时完成人眼结构三维模型成像和手术实施过程观察。It can be understood that the present invention adopts a two-dimensional galvanometer scanning unit (43), and the deflection speed of the galvanometer is extremely fast, so the entire scanning speed is greatly improved, resulting in fast imaging speed and short imaging time, which means that it can generate information that can provide information about ophthalmology. Timely and therefore useful images of the surgical progress that are fed back to the physician allow the physician to modify the surgical process in response to the feedback, which can be observed in real time while imaging of human eye structures is performed. During femtosecond laser-assisted ophthalmic surgery, doctors can observe the patient's surgical process in real time. At the same time, the two optical coherence tomography measurement systems work in coordination to image the human eye structure in real time, and can simultaneously complete the three-dimensional model imaging of the human eye structure and the observation of the surgical implementation process. .
所述的参考束和所述图像束在所述干涉仪(3)处进行相干产生相干光传输至所述探测单元(2),所述探测单元2检测所述相干光并通过所述电信号通路10传输至所述的数据采集分析单元6,生成图像信息传递至所述的图像显示单元(8)显示图像信息。The reference beam and the image beam are coherent at the interferometer (3) to generate coherent light, which is transmitted to the detection unit (2), and the
所述的控制单元(7)根据所述的图像显示单元(8)生成的图像信息生成控制信号传递至整个可降光路色散的光学相干成像系统进行实时调整。The control unit (7) generates a control signal according to the image information generated by the image display unit (8) and transmits the control signal to the entire optical coherent imaging system capable of reducing optical path dispersion for real-time adjustment.
进一步地,所述成像系统的成像时间为0.01-0.1 秒。Further, the imaging time of the imaging system is 0.01-0.1 seconds.
进一步地,所述成像系统的帧率为 50-100 帧/秒。Further, the frame rate of the imaging system is 50-100 frames per second.
可以理解的是,实况视频图像通常使用的刷新速率是约24帧/秒。因此,50-100帧/秒的刷新速率或帧率提供图像的成像系统可以提供高分辨率的实况图像给医生。而帧率或刷新速率远小于20到25帧/秒的系统可能不被视为实况视频成像,而是被视为不稳定、跳跃图像,可能甚至使医生从眼科手术分散注意力。It will be appreciated that the refresh rate typically used for live video images is about 24 frames per second. Therefore, an imaging system that provides images at a refresh rate or frame rate of 50-100 frames per second can provide high resolution live images to the physician. And systems with frame rates or refresh rates much less than 20 to 25 frames per second may not be considered live video imaging, but rather shaky, skipping images that may even distract doctors from eye surgery.
进一步地,所述成像系统的成像深度为8mm。所述成像系统的成像分辨率为5μm,解决现有技术中无法兼顾深度、高分辨率的人眼结构成像的问题,可实现术前高精度检测,术中全眼实时成像,提高手术的精确性和安全性。Further, the imaging depth of the imaging system is 8mm. The imaging resolution of the imaging system is 5 μm, which solves the problem that the prior art cannot take into account the depth and high-resolution imaging of human eye structures, can achieve high-precision preoperative detection, intraoperative real-time imaging of the whole eye, and improve the accuracy of surgery sex and safety.
本申请提供的可降光路色散的光学相干成像系统,采用偏振光成像技术,通过光纤起偏器和偏振耦合器的使用构建协调工作的可降光路色散的光学相干成像系统,不易受到自然环境中杂散光的干扰,降低了整个光路的色散,也大大降低了对光纤色散性能的要求,降低了技术方案实时的难度和成本,提高了成像信号强度和信噪比,提高了检测的精确度和实施手术的安全性。The optical coherent imaging system with reduced optical path dispersion provided by the present application adopts polarized light imaging technology, and a coordinated optical coherent imaging system with reduced optical path dispersion is constructed through the use of optical fiber polarizers and polarized couplers, which is not easily affected by the natural environment. The interference of stray light reduces the dispersion of the entire optical path, greatly reduces the requirements for fiber dispersion performance, reduces the difficulty and cost of real-time technical solutions, improves imaging signal strength and signal-to-noise ratio, and improves detection accuracy and The safety of performing the surgery.
实施例2Example 2
本申请还提供了一种可降光路色散的光学相干成像系统的成像方法,包括下述步骤:The present application also provides an imaging method of an optical coherent imaging system capable of reducing optical path dispersion, comprising the following steps:
步骤S110:所述光源(1)生成扫描波长束经过所述干涉仪(3)分为图像束和参考束;Step S110: The light source (1) generates a scanning wavelength beam that is divided into an image beam and a reference beam by the interferometer (3);
步骤S120:所述参考束通过所述光纤传输线路9依次进入所述第一起偏器(51)、所述第二起偏器(52)及所述反射镜(53),所述参考束再依次经所述反射镜(53)、所述第二起偏器(52)及所述第一起偏器(51)返回至所述干涉仪(3)Step S120 : the reference beam enters the first polarizer ( 51 ), the second polarizer ( 52 ) and the mirror ( 53 ) in sequence through the optical fiber transmission line 9 . Return to the interferometer (3) through the mirror (53), the second polarizer (52) and the first polarizer (51) in sequence
步骤S130:所述图像束依次经所述第一准直透镜(41)、所述偏振耦合器(42)、所述二维振镜扫描单元(43)、所述二向色镜(44)、所述第二准直透镜(45)、所述色散补偿器(46)及所述聚焦透镜(47)聚集于眼睛处,并由所述眼睛处将所述图像束返回至所述干涉仪(3)。Step S130: the image beam passes through the first collimating lens (41), the polarization coupler (42), the two-dimensional galvanometer scanning unit (43), and the dichroic mirror (44) in sequence , the second collimating lens (45), the dispersion compensator (46) and the focusing lens (47) are collected at the eye, and the image beam is returned from the eye to the interferometer (3).
步骤S140:所述的参考束和所述图像束在所述干涉仪(3)处进行相干产生相干光传输至所述探测单元(2),所述探测单元2检测所述相干光并通过所述电信号通路10传输至所述的数据采集分析单元6,生成图像信息传递至所述的图像显示单元(8)显示图像信息。Step S140: The reference beam and the image beam are coherent at the interferometer (3) to generate coherent light and transmit it to the detection unit (2), and the
步骤S150:所述的控制单元(7)根据所述的图像显示单元(8)生成的图像信息生成控制信号传递至整个可降光路色散的光学相干成像系统进行实时调整。Step S150: The control unit (7) generates a control signal according to the image information generated by the image display unit (8) and transmits the control signal to the entire optical coherent imaging system capable of reducing optical path dispersion for real-time adjustment.
本申请提供的光学相干成像方法,采用偏振光成像技术,通过光纤起偏器和偏振耦合器的使用构建协调工作的可降光路色散的光学相干成像系统,不易受到自然环境中杂散光的干扰,降低了整个光路的色散,也大大降低了对光纤色散性能的要求,降低了技术方案实时的难度和成本,提高了成像信号强度和信噪比,提高了检测的精确度和实施手术的安全性。The optical coherent imaging method provided by this application adopts polarized light imaging technology, and constructs a coordinated optical coherent imaging system with reduced optical path dispersion through the use of optical fiber polarizers and polarized couplers, which is not easily disturbed by stray light in the natural environment, It reduces the dispersion of the entire optical path, greatly reduces the requirements for fiber dispersion performance, reduces the difficulty and cost of real-time technical solutions, improves the imaging signal strength and signal-to-noise ratio, and improves the accuracy of detection and the safety of surgery. .
以上仅为本申请的实施例而已,并不用于限制本申请。对于本领域技术人员来说,本申请可以有各种更改和变化。凡在本申请的精神和原理之内所作的任何修改、等同替换、改进等,均应包含在本申请的权利要求范围之内。The above are merely examples of the present application, and are not intended to limit the present application. Various modifications and variations of this application are possible for those skilled in the art. Any modification, equivalent replacement, improvement, etc. made within the spirit and principle of this application shall be included within the scope of the claims of this application.
Claims (7)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202110239421.XA CN112596256A (en) | 2021-03-04 | 2021-03-04 | Optical coherent imaging system capable of reducing optical path dispersion and imaging method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202110239421.XA CN112596256A (en) | 2021-03-04 | 2021-03-04 | Optical coherent imaging system capable of reducing optical path dispersion and imaging method |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CN112596256A true CN112596256A (en) | 2021-04-02 |
Family
ID=75210316
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN202110239421.XA Pending CN112596256A (en) | 2021-03-04 | 2021-03-04 | Optical coherent imaging system capable of reducing optical path dispersion and imaging method |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN112596256A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN117870574A (en) * | 2024-03-13 | 2024-04-12 | 广东普洛宇飞生物科技有限公司 | Laser optical device capable of correcting in real time and correction method thereof |
| CN117870575A (en) * | 2024-03-13 | 2024-04-12 | 广东普洛宇飞生物科技有限公司 | Rapid imaging system and imaging method for correcting wave front in real time |
Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR20050043164A (en) * | 2003-11-05 | 2005-05-11 | 한국전기연구원 | Oct(optical coherence tomography) system using a ccd(charge coupled device) camera |
| CN101711667A (en) * | 2009-11-26 | 2010-05-26 | 浙江大学 | Quick detecting method and system for acousto-optic gated spectra of spectral domain OCT |
| CN103284687A (en) * | 2009-10-23 | 2013-09-11 | 佳能株式会社 | Ophthalmology imaging device and ophthalmology imaging method |
| CN111657847A (en) * | 2013-06-20 | 2020-09-15 | 赛莱特私人有限公司 | Device and method for analyzing a sample |
-
2021
- 2021-03-04 CN CN202110239421.XA patent/CN112596256A/en active Pending
Patent Citations (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR20050043164A (en) * | 2003-11-05 | 2005-05-11 | 한국전기연구원 | Oct(optical coherence tomography) system using a ccd(charge coupled device) camera |
| CN103284687A (en) * | 2009-10-23 | 2013-09-11 | 佳能株式会社 | Ophthalmology imaging device and ophthalmology imaging method |
| CN101711667A (en) * | 2009-11-26 | 2010-05-26 | 浙江大学 | Quick detecting method and system for acousto-optic gated spectra of spectral domain OCT |
| CN111657847A (en) * | 2013-06-20 | 2020-09-15 | 赛莱特私人有限公司 | Device and method for analyzing a sample |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN117870574A (en) * | 2024-03-13 | 2024-04-12 | 广东普洛宇飞生物科技有限公司 | Laser optical device capable of correcting in real time and correction method thereof |
| CN117870575A (en) * | 2024-03-13 | 2024-04-12 | 广东普洛宇飞生物科技有限公司 | Rapid imaging system and imaging method for correcting wave front in real time |
| CN117870574B (en) * | 2024-03-13 | 2024-05-14 | 广东普洛宇飞生物科技有限公司 | Laser optical device capable of correcting in real time and correction method thereof |
| CN117870575B (en) * | 2024-03-13 | 2024-06-04 | 广东普洛宇飞生物科技有限公司 | Rapid imaging system and imaging method for correcting wave front in real time |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US8469514B2 (en) | Image sensing apparatus using optical coherence tomography and control method therefor | |
| CN105147241B (en) | Method and system based on double space carrier frequency technique extension OCT image depth | |
| US8801178B2 (en) | Fundus photographing apparatus | |
| CN101791213B (en) | Optical tomographic imaging apparatus | |
| US10105050B2 (en) | Adaptive optics apparatus, adaptive optics method, and imaging apparatus | |
| CN100488440C (en) | Common channel type endoscopic optical coherent chromatography imaging method and system | |
| CN104337498B (en) | Oct | |
| CN112596256A (en) | Optical coherent imaging system capable of reducing optical path dispersion and imaging method | |
| JP6525777B2 (en) | Ophthalmic surgery system | |
| CN102860817A (en) | Laser scanning confocal ophthalmoscope device based on double wave front corrector | |
| CN112493982A (en) | OCT structure and blood flow imaging's device in art | |
| CN114869221A (en) | A dispersion-balanced swept-frequency OCT fundus high-resolution imaging system | |
| JP5545984B2 (en) | Fundus imaging device with wavefront compensation | |
| US11806077B2 (en) | Ophthalmologic apparatus, and ophthalmologic information processing apparatus | |
| CN102297655A (en) | Testing method for performing bidirectional positioning and synchronous testing on fiber end face | |
| US20150157204A1 (en) | Light Source Modulation for a Scanning Microscope | |
| JP7178683B2 (en) | ophthalmic equipment | |
| JP7726923B2 (en) | Assembly for performing optical coherence tomography | |
| CN112603255A (en) | Optical coherent imaging system and imaging method capable of eliminating inherent noise | |
| CN112587084A (en) | Optical coherent imaging system with real-time adjustable imaging depth | |
| CN105832305B (en) | Wear-type optical coherence tomography system for free movement animal | |
| CN201101518Y (en) | Common channel type endoscopic optical coherent chromatography imaging system | |
| JP2020536689A (en) | Methods and systems for monitoring motor control functions | |
| CN114668582B (en) | Ophthalmologic light source operation system | |
| JP2015016387A (en) | Optical coherence tomography apparatus, control method and program for optical coherence tomography apparatus |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PB01 | Publication | ||
| PB01 | Publication | ||
| SE01 | Entry into force of request for substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| RJ01 | Rejection of invention patent application after publication |
Application publication date: 20210402 |
|
| RJ01 | Rejection of invention patent application after publication |