CN117288684A - Cone-shaped optical fiber single-pixel imaging system and method based on compressed sensing - Google Patents

Cone-shaped optical fiber single-pixel imaging system and method based on compressed sensing Download PDF

Info

Publication number
CN117288684A
CN117288684A CN202311081474.9A CN202311081474A CN117288684A CN 117288684 A CN117288684 A CN 117288684A CN 202311081474 A CN202311081474 A CN 202311081474A CN 117288684 A CN117288684 A CN 117288684A
Authority
CN
China
Prior art keywords
optical fiber
multimode
imaging
tapered
compressed sensing
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
Application number
CN202311081474.9A
Other languages
Chinese (zh)
Inventor
陈娜
孙梦
商娅娜
刘书朋
刘勇
庞拂飞
王廷云
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
SHANGHAI UNIVERSITY
Original Assignee
SHANGHAI UNIVERSITY
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by SHANGHAI UNIVERSITY filed Critical SHANGHAI UNIVERSITY
Priority to CN202311081474.9A priority Critical patent/CN117288684A/en
Publication of CN117288684A publication Critical patent/CN117288684A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • 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
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • GPHYSICS
    • G01MEASURING; TESTING
    • 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
    • G01N21/01Arrangements or apparatus for facilitating the optical investigation
    • GPHYSICS
    • G01MEASURING; TESTING
    • 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
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N2021/1765Method using an image detector and processing of image signal

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Microscoopes, Condenser (AREA)

Abstract

The invention discloses a tapered optical fiber single-pixel imaging system and a tapered optical fiber single-pixel imaging method based on compressed sensing, wherein the tapered optical fiber single-pixel imaging system and the tapered optical fiber single-pixel imaging method based on compressed sensing comprise the following steps: the system comprises a conical multimode fiber, a two-dimensional micrometer mobile station, an imaging module, a signal collection module and a point detector; the conical multimode optical fiber is arranged on the two-dimensional micrometer mobile station, the position of the conical multimode optical fiber is adjusted through the two-dimensional micrometer mobile station, and the laser light source emits multimode interference speckles after being transmitted by the conical multimode optical fiber and is used for irradiating and modulating sample information. The tail end core diameter of the conical multimode fiber can be controlled at a micron level, and the speckle illumination field of view is reduced by reducing the tail end core diameter so as to realize imaging of a sample with smaller size and realize calculation super-resolution imaging by combining a compressed sensing technology. The imaging limit of the method is far higher than that of a common multimode optical fiber.

Description

基于压缩感知的锥形光纤单像素成像系统及方法Tapered optical fiber single-pixel imaging system and method based on compressed sensing

技术领域Technical field

本发明属于成像技术领域,尤其是涉及一种基于压缩感知的锥形光纤单像素成像系统及方法及方法。The invention belongs to the field of imaging technology, and in particular relates to a tapered optical fiber single-pixel imaging system and method based on compressed sensing.

背景技术Background technique

早在几个世纪以来,光学显微镜一直作为化学、生物等材料不可替代重要表征手段。随着技术的发展,光学成像一直向更微小尺寸突破,而阿贝尔衍射极限表明远场成像系统的分辨率一直受光波长和成像系统的数值孔径限制。为了克服远场衍射极限带来的限制,一系列超分辨成像技术得到突破和发展,其中包括近场光学显微镜,其绕开了远场的限制,利用光纤探针将光源变为纳米级光源并将其深入样品的近场区域即小于一个光波长距离内进行探测,通过扫描的方式实现一定区域的超分辨成像,该技术经常被用于分子或化学材料的成像。此外,基于荧光特性的超分辨显微镜技术在远场观察中具有较好的优势,先后出现光激活定位显微镜(PALM)、随机光学重构显微镜(STORM)、受激发射损耗(STED)显微技术、基于光学闪烁的超分辨成像(SOFI)、基于闪烁半径的超分辨成像(SRRF)。基于荧光分子的超分辨显微镜更加适用于分析生物切片,而基于光纤的成像系统展现出了在深组织成像的巨大优势,其微小的尺寸和较好的韧性可以灵活地深入活体生物内部进行内窥成像。For centuries, optical microscopy has been an irreplaceable and important means of characterization of chemical, biological and other materials. With the development of technology, optical imaging has been breaking through to smaller sizes, and the Abelian diffraction limit shows that the resolution of far-field imaging systems has always been limited by the wavelength of light and the numerical aperture of the imaging system. In order to overcome the limitations caused by the far-field diffraction limit, a series of super-resolution imaging technologies have been broken through and developed, including near-field optical microscopy, which bypasses the limitations of the far-field and uses optical fiber probes to change the light source into a nanoscale light source and It is detected deep into the near-field region of the sample, that is, within a distance of less than one optical wavelength, and super-resolution imaging of a certain area is achieved by scanning. This technology is often used for imaging molecules or chemical materials. In addition, super-resolution microscopy technology based on fluorescence characteristics has good advantages in far-field observation. Photoactivated localization microscopy (PALM), stochastic optical reconstruction microscopy (STORM), and stimulated emission depletion (STED) microscopy have successively appeared. , super-resolution imaging based on optical scintillation (SOFI), super-resolution imaging based on scintillation radius (SRRF). Super-resolution microscopes based on fluorescent molecules are more suitable for analyzing biological slices, while optical fiber-based imaging systems have shown great advantages in deep tissue imaging. Their tiny size and good toughness can flexibly penetrate deep into living organisms for endoscopic observation. Imaging.

目前基于光纤束的内窥成像技术即内窥镜已经较为成熟的运用到了医疗行业。光纤束本身是由数千个光纤组成,其在尺寸上还不够微型化,其成像的分辨率依赖于光纤的数量,光纤与光纤之间的空隙容易导致成像的伪影。近几年,基于单根光纤成像的技术逐渐被广泛研究,在小型化上比光纤束更加具有优势。其成像手段主要是利用波前整形的复杂波前使其在多模光纤输出端产生不同位置的激光聚焦点,由此进行栅格扫描成像。为了简化波前整形的复杂度以及提高成像速度,基于压缩感知(CS)重构算法的光纤散斑照明成像方法也得到了进一步的发展,该成像方法的本质和单像素相机一致,不同之处在于调制光斑不是简单依赖于数字微镜(DMD)或空间光调制器(SLM),而是利用多模光纤的模式干涉效应或光纤端面镀膜产生的散斑作为照明的调制光斑,最后利用桶探测器进行一维强度信号的收集。且基于传统波前整形的单根多模光纤成像技术的成像分辨率受限于光纤本身的衍射极限,无法进一步提高成像分辨率。相反,CS技术基于原始信号的稀疏性,可以重构出远多于压缩信号的数据;同理,对于稀疏图像信号,也可以重构出比远场图像分辨率更高的图像。最近,有仿真详细讨论了基于CS技术的散斑照明单像素成像的分辨率极限,限制成像分辨率的本质因素是样本的稀疏性。此外,数据测量次数、测量散斑的选取以及重建算法的性能也会极大地影响成像质量,从而影响成像分辨率。在实验层面,近期有研究通过激光激励多模光纤入射端纤芯的不同位置产生多个干涉散斑对荧光小球进行调制照明和荧光信号探测,最后通过压缩感知重构算法重构荧光图像,实现了亚微米尺寸的成像,其成功超过了多模光纤的衍射极限。然而,进一步提高基于光纤内窥成像分辨率是具有极大意义的,有助于观察生物或组织体中更加微观地活动。At present, endoscopic imaging technology based on optical fiber bundles, namely endoscopes, has been relatively maturely used in the medical industry. The fiber bundle itself is composed of thousands of optical fibers, which are not miniaturized in size. The imaging resolution depends on the number of optical fibers. The gaps between optical fibers can easily cause imaging artifacts. In recent years, imaging technology based on a single optical fiber has gradually been widely studied, and it has more advantages than fiber bundles in terms of miniaturization. The imaging method mainly uses the complex wavefront of wavefront shaping to generate laser focus points at different positions at the output end of the multimode fiber, thereby performing raster scanning imaging. In order to simplify the complexity of wavefront shaping and improve the imaging speed, the optical fiber speckle illumination imaging method based on the compressed sensing (CS) reconstruction algorithm has also been further developed. The essence of this imaging method is the same as that of a single-pixel camera. The differences are The modulated light spot does not simply rely on the digital micromirror (DMD) or the spatial light modulator (SLM), but uses the modal interference effect of multi-mode fiber or the speckle generated by the fiber end-face coating as the modulated light spot of the illumination, and finally uses barrel detection The detector collects one-dimensional intensity signals. Moreover, the imaging resolution of single multimode fiber imaging technology based on traditional wavefront shaping is limited by the diffraction limit of the fiber itself, and cannot further improve the imaging resolution. On the contrary, CS technology is based on the sparseness of the original signal and can reconstruct far more data than the compressed signal. Similarly, for sparse image signals, it can also reconstruct images with higher resolution than far-field images. Recently, simulations have discussed in detail the resolution limit of single-pixel imaging with speckle illumination based on CS technology. The essential factor limiting the imaging resolution is the sparsity of the sample. In addition, the number of data measurements, the selection of measurement speckles, and the performance of the reconstruction algorithm will also greatly affect the imaging quality and thus the imaging resolution. At the experimental level, recent research has used laser excitation to produce multiple interference speckles at different positions of the incident end core of multi-mode optical fibers to modulate illumination and detect fluorescence signals on fluorescent beads, and finally reconstruct the fluorescence image through a compressed sensing reconstruction algorithm. Imaging of submicron dimensions was achieved, which successfully exceeded the diffraction limit of multimode optical fiber. However, it is of great significance to further improve the resolution of fiber-optic endoscopic imaging, which will help to observe more microscopic activities in organisms or tissues.

发明内容Contents of the invention

本发明所要解决的技术问题是:针对现有技术中的基于单根光纤成像的分辨率有待进一步提高,提供一种基于压缩感知的锥形光纤单像素成像系统及方法及方法,通过将多模光纤制备成锥形多模光纤的方法来缩小成像视场进而有效地提高成像分辨率。The technical problem to be solved by the present invention is to provide a tapered optical fiber single-pixel imaging system and method based on compressed sensing in order to further improve the resolution of single-fiber imaging in the prior art. By combining multi-mode The optical fiber is prepared into a tapered multi-mode optical fiber to reduce the imaging field of view and thereby effectively improve the imaging resolution.

本发明通过下述技术方案实现:The present invention is realized through the following technical solutions:

一方面,本发明提供了一种基于压缩感知的锥形光纤单像素成像系统及方法,包括:锥形多模光纤、二维微米移动台、成像模块、信号收集模块和点探测器;锥形多模光纤安装在二维微米移动台上,通过二维微米移动台调节锥形多模光纤的位置,激光光源经过锥形多模光纤传输后出射随空间位置变化的多模干涉散斑,用于照射并调制样品信息。On the one hand, the present invention provides a tapered optical fiber single-pixel imaging system and method based on compressed sensing, including: tapered multi-mode optical fiber, two-dimensional micron mobile stage, imaging module, signal collection module and point detector; tapered The multimode fiber is installed on a two-dimensional micron moving stage. The position of the tapered multimode fiber is adjusted through the two-dimensional micron moving stage. After the laser light source is transmitted through the tapered multimode fiber, it emits multimode interference speckles that change with the spatial position. to irradiate and modulate sample information.

锥形多模光纤是由多模光纤被横向拉锥并从腰区切割制成。多模光纤在给定工作波长上传输多种模式。二维微米移动台是通过移动固定在其上面的光纤来改变激光入射位置,进而产生空间调制的随机多模干涉散斑,二维微米移动台最小移动距离不大于0.1μm,可移动方向至少为x-y两方向。Tapered multimode fiber is made by transversely tapering a multimode fiber and cutting it from the waist region. Multimode fiber transmits multiple modes at a given operating wavelength. The two-dimensional micron mobile stage changes the laser incident position by moving the optical fiber fixed on it, thereby generating spatially modulated random multi-mode interference speckles. The minimum moving distance of the two-dimensional micron mobile stage is not greater than 0.1μm, and the movable direction is at least x-y directions.

成像模块包括物镜和相机,用于对样品进行成像观察激光散斑照射在样品上的照射情况。The imaging module includes an objective lens and a camera, which is used to image the sample and observe the illumination of the laser speckle on the sample.

信号收集模块包括物镜和分束镜点探测器。信号收集模块为物镜将散斑调制样品后的光强信息聚焦并用分束镜分开一路光由点探测器收集。The signal collection module includes an objective lens and a beam splitter point detector. The signal collection module uses the objective lens to focus the light intensity information after speckle modulation of the sample and uses a beam splitter to separate a path of light and collect it with a point detector.

点探测器用于探测调制散斑用于样品后的一维光强信息,并通过压缩感知重构算法对欠采样的一维光强进行二维图像重构;The point detector is used to detect the one-dimensional light intensity information after the modulated speckle is applied to the sample, and reconstruct the two-dimensional image of the undersampled one-dimensional light intensity through the compressed sensing reconstruction algorithm;

一种基于压缩感知和单像素成像的锥形多模光纤超分辨成像方法,其特征在于以下包括以下步骤:S1产生多模干涉散斑,S2产生空间调制散斑照明源,S3调整散斑照明样品的视场,S4表征调制散斑序列信息,S5收集光强信息并重构成像。A tapered multi-mode optical fiber super-resolution imaging method based on compressed sensing and single-pixel imaging, which is characterized by including the following steps: S1 generates multi-mode interference speckles, S2 generates spatially modulated speckle illumination sources, and S3 adjusts the speckle illumination. The field of view of the sample, S4 represents the modulated speckle sequence information, and S5 collects the light intensity information and reconstructs the imaging.

具体步骤过程如下The specific steps are as follows

S1:激光光源入射锥形多模光纤输入端面经一段距离传输后产生多种模式干涉的激光散斑;S1: The laser light source is incident on the input end face of the tapered multi-mode fiber and is transmitted over a distance to produce laser speckles of multiple modes of interference;

S2:利用二维微米台来控制锥形多模光纤输入面移动产生空间调制的随机激光散斑;S2: Use a two-dimensional micron platform to control the movement of the tapered multimode optical fiber input surface to generate spatially modulated random laser speckles;

S3:锥形多模光纤输出端直接靠近样品照明,通过控制锥形多模光纤输出端和样品的相对距离来控制照明视场范围的变化,由此实现不同放大倍数的成像;S3: The output end of the tapered multimode optical fiber is directly close to the sample illumination. By controlling the relative distance between the output end of the tapered multimode optical fiber and the sample, the change in the illumination field of view is controlled, thereby achieving imaging with different magnifications;

S4:利用物镜和相机组成的成像模块精准控制调制散斑的照射位置和视场大小并利用相机预先表征散斑信息作为后续图像重构的输入参数;S4: Use the imaging module composed of the objective lens and the camera to accurately control the illumination position and field of view size of the modulated speckle, and use the camera to pre-characterize the speckle information as an input parameter for subsequent image reconstruction;

S5:信号收集模块对调制散斑作用于样品后的光强信息进行聚焦并通过点探测器收集,通过压缩感知重构算法根据探测的光强和散斑信息重构出样品图像。S5: The signal collection module focuses the light intensity information after the modulated speckle acts on the sample and collects it through the point detector. The sample image is reconstructed based on the detected light intensity and speckle information through the compressed sensing reconstruction algorithm.

本发明将锥形多模光纤端面固定在二维微米台上;控制微米台移动来改变激光在锥形多模光纤端面的激励位置;产生空间调制的随机多模干涉散斑;通过点探测器收集调制散斑作用于样品后的光强,基于散斑和已探测的光强,并利用压缩感知重构算法对样品图像信息进行重构。与现有技术相比,具有以下优点:The invention fixes the end face of the tapered multi-mode optical fiber on a two-dimensional micron platform; controls the movement of the micron platform to change the excitation position of the laser on the end face of the tapered multi-mode optical fiber; generates spatially modulated random multi-mode interference speckles; and passes the point detector The light intensity after the modulated speckle acts on the sample is collected. Based on the speckle and the detected light intensity, the sample image information is reconstructed using the compressed sensing reconstruction algorithm. Compared with existing technology, it has the following advantages:

(1)传统基于压缩感知和单像素成像的多模光纤成像技术由于其固定的末端芯径,其照射样品时无法进一步缩小照明视场,而本发明提出将多模光纤制备成锥形多模光纤,通过制备不同末端芯径的锥形多模光纤灵活调控最小照明视场范围。(1) Due to its fixed end core diameter, the traditional multi-mode optical fiber imaging technology based on compressed sensing and single-pixel imaging cannot further reduce the illumination field of view when irradiating the sample. However, the present invention proposes to prepare the multi-mode optical fiber into a tapered multi-mode Optical fiber can flexibly control the minimum illumination field of view by preparing tapered multi-mode optical fibers with different end core diameters.

(2)传统基于压缩感知和单像素成像的多模光纤成像技术提高成像分辨率的程度有限,而本发明使用的锥形多模光纤在保留了多模散斑特征的同时缩小了照明视场,在基于CS的计算超分辨成像中表现出了比普通多模光纤更大的优势。(2) Traditional multi-mode optical fiber imaging technology based on compressed sensing and single-pixel imaging has limited improvement in imaging resolution. However, the tapered multi-mode optical fiber used in the present invention reduces the illumination field of view while retaining the multi-mode speckle characteristics. , showing greater advantages than ordinary multimode optical fiber in CS-based computational super-resolution imaging.

附图说明Description of drawings

图1本发明的锥形多模光纤成像系统光路示意图;Figure 1 is a schematic diagram of the optical path of the tapered multi-mode optical fiber imaging system of the present invention;

图2为本发明结合压缩感知和单像素成像技术的成像原理图;Figure 2 is an imaging principle diagram of the present invention combining compressed sensing and single-pixel imaging technology;

图3为本发明制备的锥形多模光纤的光学图。Figure 3 is an optical diagram of the tapered multimode optical fiber prepared by the present invention.

具体实施方式Detailed ways

为了使本发明的目的、技术方案及优点更加清楚,以下通过具体实施,并结合附图,对本发明进一步详细说明。In order to make the purpose, technical solutions and advantages of the present invention clearer, the present invention will be further described in detail below through specific implementation and in conjunction with the accompanying drawings.

实施例一Embodiment 1

传统基于波前整形的单根多模光纤成像因其扫描成像的特点,其成像速度较慢且成像分辨率受光纤衍射极限限制。而基于压缩感知单像素成像的单根多模光纤成像虽然提高了成像效率并达到了亚微米尺寸的成像,但其成像视场范围无法进一步缩小以及成像分辨率仍有待进一步提高。Traditional single multimode fiber imaging based on wavefront shaping has slow imaging speed and imaging resolution is limited by the diffraction limit of the fiber due to its scanning imaging characteristics. Although single multi-mode fiber imaging based on compressed sensing single-pixel imaging improves imaging efficiency and achieves sub-micron size imaging, its imaging field of view cannot be further reduced and the imaging resolution still needs to be further improved.

本实施例公开了一种基于压缩感知和单像素成像的锥形多模光纤成像系统,将多模光纤制备成末端芯径小于原尺寸并灵活控制芯径尺寸为微米级别。并将锥形多模光纤与二维微米移动台结合产生空间调制的多模干涉散斑作为调制光。锥形多模光纤在保留了调制照明散斑的同时减小了最小成像视场,有效地实现了对更小尺寸样品的成像并结合CS技术实现计算超分辨成像。This embodiment discloses a tapered multi-mode optical fiber imaging system based on compressed sensing and single-pixel imaging. The multi-mode optical fiber is prepared so that the end core diameter is smaller than the original size and the core diameter size is flexibly controlled to the micron level. The tapered multimode optical fiber is combined with a two-dimensional micron moving stage to generate spatially modulated multimode interference speckles as modulated light. The tapered multimode fiber retains the modulated illumination speckle while reducing the minimum imaging field of view, effectively achieving imaging of smaller size samples and combining with CS technology to achieve computational super-resolution imaging.

本实施例具体的系统模块图如图1所示,包括:The specific system module diagram of this embodiment is shown in Figure 1, including:

窄带激光器(Laser);本实施例中使用532nm激光器作为光源通过聚焦光路聚焦到锥形多模光纤输入端面,根据成像波段的需要可以选择不同波段的激光器;Narrowband laser (Laser); in this embodiment, a 532nm laser is used as the light source and focused on the input end face of the tapered multi-mode optical fiber through the focusing optical path. Lasers of different bands can be selected according to the needs of the imaging band;

锥形多模光纤(Tapered MMF);由普通多模光纤横向拉锥并从腰区切割而制得,光纤的末端呈圆锥形,末端纤芯直径从几微米到几十微米不等,图3给出了三种不同尺寸的锥形多模光纤光学图;本实施例中利用锥形多模光纤产生的激光散斑作为样品成像的调制光源;Tapered multimode optical fiber (Tapered MMF) is made by transversely tapering ordinary multimode optical fiber and cutting it from the waist area. The end of the optical fiber is conical, and the end core diameter ranges from a few microns to tens of microns, Figure 3 The optical diagrams of three different sizes of tapered multimode optical fibers are given; in this embodiment, the laser speckle generated by the tapered multimode optical fiber is used as the modulated light source for sample imaging;

二维微米移动台(XY stage);可程控的具有x-y两个移动方向的微米台,最小移动精度可达到0.1μm;本实施例中用于移动锥形多模光纤的入射端面来改变激光激励位置产生空间调制的多模干涉散斑;Two-dimensional micron moving stage (XY stage); a programmable micron stage with two moving directions of x-y, the minimum moving accuracy can reach 0.1μm; in this embodiment, it is used to move the incident end face of the tapered multi-mode fiber to change the laser excitation Position produces spatially modulated multimode interference speckles;

成像模块;位于样品之后,由物镜(OL)和相机(CCD)组成;本实施例中用于对样品进行成像来观察激光散斑照射在样品上的照射情况;Imaging module; located behind the sample, consisting of an objective lens (OL) and a camera (CCD); in this embodiment, it is used to image the sample to observe the irradiation of the laser speckle on the sample;

信号收集模块;位于样品之后,由物镜(OL)、分束镜(BS)和点探测器(PD);本实施例中用于对散斑作用于样品之后的光强信号进行聚焦并由点探测器收集。Signal collection module; located behind the sample, consists of an objective lens (OL), a beam splitter (BS) and a point detector (PD); in this embodiment, it is used to focus the light intensity signal after the speckle acts on the sample and use the point detector to detector collection.

根据本发明实施例提出的基于压缩感知的锥形光纤单像素成像系统及方法,将多模光纤制备成末端芯径小于原尺寸并灵活控制芯径尺寸为微米级。并将锥形多模光纤与二维微米移动台结合产生空间调制的多模干涉散斑本作为调制光。锥形多模光纤在保留了调制照明散斑的同时减小了最小成像视场,有效地实现了对更小尺寸样品的成像并结合CS技术实现计算超分辨成像。According to the compressed sensing-based tapered optical fiber single-pixel imaging system and method proposed by embodiments of the present invention, the multi-mode optical fiber is prepared so that the end core diameter is smaller than the original size and the core diameter size is flexibly controlled to the micron level. The tapered multimode optical fiber is combined with a two-dimensional micron moving stage to generate spatially modulated multimode interference speckles as modulated light. The tapered multimode fiber retains the modulated illumination speckle while reducing the minimum imaging field of view, effectively achieving imaging of smaller size samples and combining with CS technology to achieve computational super-resolution imaging.

实施例二Embodiment 2

本实施例公开了一种基于压缩感知和单像素成像的锥形多模光纤超分辨成像方法,本实施例是在实施例一中的成像系统基础上实现的成像方法,具体原理如图2所示,具体步骤如下:This embodiment discloses a tapered multi-mode optical fiber super-resolution imaging method based on compressed sensing and single-pixel imaging. This embodiment is an imaging method implemented based on the imaging system in Embodiment 1. The specific principle is shown in Figure 2 shown, the specific steps are as follows:

S1:激光光源入射锥形多模光纤输入端面后经一段距离传输后产生多种模式干涉的激光散斑;S1: The laser light source is incident on the input end face of the tapered multi-mode optical fiber and then propagates over a certain distance to produce laser speckles of multiple modes of interference;

S2:利用二维微米台来控制锥形多模光纤输入面移动产生空间调制的随机激光散斑;S2: Use a two-dimensional micron platform to control the movement of the tapered multimode optical fiber input surface to generate spatially modulated random laser speckles;

对二维微米台进行二维路径规划扫描,固定在微米台上的锥形多模光纤端面进行相应的二维路径扫描,由此激光入射点相对发生扫描;扫描路径的总范围不得超过纤芯尺寸的范围,实施例中随扫描产生的一系列照明所需的散斑。所有的照明散斑对应于CS理论中的测量矩阵Ф,图2有所示意。A two-dimensional path planning scan is performed on the two-dimensional micron stage. The tapered multi-mode optical fiber end face fixed on the micron stage is scanned with the corresponding two-dimensional path, so that the laser incident point is relatively scanned; the total range of the scanning path must not exceed the fiber core. The range of sizes, speckles required for the series of illumination generated with the scan in the example. All illumination speckles correspond to the measurement matrix Ф in CS theory, as shown in Figure 2.

S3:锥形多模光纤输出端直接靠近样品照明,通过控制锥形多模光纤输出端和样品的相对距离来控制照明视场范围的变化,由此实现不同放大倍数的成像;S3: The output end of the tapered multimode optical fiber is directly close to the sample illumination. By controlling the relative distance between the output end of the tapered multimode optical fiber and the sample, the change in the illumination field of view is controlled, thereby achieving imaging with different magnifications;

S4:利用物镜和相机组成的成像模块精准控制调制散斑的照射位置和视场大小并利用相机预先表征散斑信息作为后续图像重构的输入参数;S4: Use the imaging module composed of the objective lens and the camera to accurately control the illumination position and field of view size of the modulated speckle, and use the camera to pre-characterize the speckle information as an input parameter for subsequent image reconstruction;

S5:信号收集模块对调制散斑作用于样品后的光强信息进行聚焦并通过点探测器收集,通过压缩感知重构算法根据探测的光强和散斑信息重构出样品图像;S5: The signal collection module focuses the light intensity information after the modulated speckle acts on the sample and collects it through the point detector, and reconstructs the sample image based on the detected light intensity and speckle information through the compressed sensing reconstruction algorithm;

表征后的散斑信息组成CS理论中的测量矩阵Ф,具体将每一个散斑展开成一维行向量,行向量的长度则定义为N,这里N同时对应于待测样品x的信号长度即分辨率,散斑的数量定义为M;因此测量矩阵Ф则是一个M×N的二维矩阵。由于散斑测量次数M通常远小于待测样品x的信号长度N,这就构成了CS理论中的欠采样模型,为实现计算超分辨成像打下理论基础。把点探测器测得的一维度光强信号定义为y,整个单像素探测过程就可以描述为以下数学过程:The characterized speckle information forms the measurement matrix Ф in CS theory. Specifically, each speckle is expanded into a one-dimensional row vector, and the length of the row vector is defined as N, where N also corresponds to the signal length of the sample x to be measured, that is, the resolution. rate, the number of speckles is defined as M; therefore the measurement matrix Ф is an M×N two-dimensional matrix. Since the number of speckle measurements M is usually much smaller than the signal length N of the sample x to be measured, this constitutes an undersampling model in CS theory and lays a theoretical foundation for realizing computational super-resolution imaging. Defining the one-dimensional light intensity signal measured by the point detector as y, the entire single-pixel detection process can be described as the following mathematical process:

y=Φx (1)y=Φx (1)

其中y为点探测器获得的光强信号,Ф是由照明散斑组成的测量矩阵,x为待成像样品。CS理论中对于式(1)欠定方程的求解是基于样品的稀疏性约束,这里不需要要求样品x本身稀疏,只需要其在某变换域具有稀疏特性即可。自然界大多数样品,在某些变换域都具有稀疏性,例如余弦变换域,梯度变换域等。基于样品的稀疏约束,利用CS重构算法对等式(1)进行求解,最终获得样品信号x。Among them, y is the light intensity signal obtained by the point detector, Ф is the measurement matrix composed of illumination speckles, and x is the sample to be imaged. In CS theory, the solution to the underdetermined equation of equation (1) is based on the sparsity constraint of the sample. Here, the sample x itself does not need to be sparse, but only needs to have sparse characteristics in a certain transformation domain. Most samples in nature are sparse in certain transformation domains, such as cosine transformation domain, gradient transformation domain, etc. Based on the sparse constraint of the sample, the CS reconstruction algorithm is used to solve equation (1), and finally the sample signal x is obtained.

总之,本发明将锥形多模光纤作为单像素成像的调制光产生器件,其产生调制散斑的同时又可以灵活调节最小成像视场从而可以实现更小样品的成像,之后通过相机表征散斑信息并通过点探测器收集散斑调制样品后的光强信息。最后基于CS技术对图像进行重构并完成计算超分辨成像。In short, the present invention uses a tapered multi-mode fiber as a modulated light generating device for single-pixel imaging. It generates modulated speckles and can flexibly adjust the minimum imaging field of view to achieve imaging of smaller samples. The speckles are then characterized by a camera. information and collects the light intensity information after speckle modulation of the sample through a point detector. Finally, the image is reconstructed based on CS technology and computational super-resolution imaging is completed.

在此有必要指出的是,以上实施例和试验例仅限于对本发明的技术方案做进一步的阐述和理解,不能理解为对本发明的技术方案做进一步的限定,本领域技术人员做出得非突出实质性特征和显著进步的发明创造,仍然属于本发明的保护范畴。It is necessary to point out here that the above examples and test examples are only for further elaboration and understanding of the technical solution of the present invention, and cannot be understood as further limitations of the technical solution of the present invention. Those skilled in the art will not make outstanding achievements. Inventions and creations with substantial features and significant advancements still fall within the scope of protection of the present invention.

Claims (10)

1. A tapered optical fiber single-pixel imaging system and method based on compressed sensing are characterized by comprising the following steps: the system comprises a conical multimode fiber, a two-dimensional micrometer mobile station, an imaging module, a signal collection module and a point detector; the conical multimode optical fiber is arranged on the two-dimensional micrometer mobile station, the movement of the conical multimode optical fiber is controlled by the two-dimensional micrometer mobile station, the position of the corresponding laser incident on the end face of the conical multimode optical fiber changes, and the laser source emits multimode interference speckles modulated by the spatial position after being transmitted by the conical multimode optical fiber and is used for irradiating and modulating sample information.
2. The compressed sensing based tapered fiber single-pixel imaging system and method as claimed in claim 1, wherein the tapered multimode fiber is made from multimode fiber that is tapered laterally and cut from the waist region.
3. The compressed sensing-based tapered fiber optic single-pixel imaging system and method as claimed in claim 2, wherein: multimode optical fibers transmit multiple modes at a given operating wavelength.
4. The compressed sensing-based tapered optical fiber single-pixel imaging system and method according to claim 3, wherein the two-dimensional micrometer movable stage changes the incident position of the laser by moving the optical fiber fixed on the two-dimensional micrometer movable stage, thereby generating spatially modulated random multimode interference speckle, the minimum moving distance of the two-dimensional micrometer movable stage is not more than 0.1 μm, and the movable direction is at least in the x-y directions.
5. The compressed sensing-based tapered fiber single-pixel imaging system and method as claimed in claim 4, wherein the imaging module comprises an objective lens and a camera for imaging the sample to observe the illumination of the sample by the laser speckle.
6. The compressed sensing based tapered fiber single-pixel imaging system and method of claim 5, wherein the signal collection module comprises an objective lens, a beam splitter, and a point detector.
7. The system and method for tapered fiber single-pixel imaging based on compressed sensing as claimed in claim 6, wherein the signal collection module is an objective lens for focusing the light intensity information of the speckle-modulated sample and a beam splitter for splitting a path of light for collection by the point detector.
8. The compressed sensing-based tapered optical fiber single-pixel imaging system and method according to claim 6 or 7, wherein the point detector is used for detecting one-dimensional light intensity information after modulation speckle is applied to the sample, and performing two-dimensional image reconstruction on undersampled one-dimensional light intensity through a compressed sensing reconstruction algorithm.
9. A conical multimode optical fiber super-resolution imaging method based on compressed sensing and single-pixel imaging is characterized by comprising the following steps of: s1 generates multimode interference speckle, S2 generates a space modulation speckle illumination source, S3 adjusts the field of view of a speckle illumination sample, S4 characterizes modulated speckle sequence information, and S5 collects light intensity information and reconstructs an image.
10. The method for tapered multimode fiber super-resolution imaging based on compressed sensing and single-pixel imaging as claimed in claim 9 comprises the following specific steps of
S1: the laser source enters the tapered multimode fiber input end face to be transmitted for a certain distance to generate laser speckles with multiple mode interference;
s2: controlling the movement of the input surface of the tapered multimode fiber to generate spatially modulated random laser speckles by using a two-dimensional micrometer stage;
s3: the conical multimode fiber output end is directly close to the sample for illumination, and the change of the illumination field range is controlled by controlling the relative distance between the conical multimode fiber output end and the sample, so that imaging with different magnification is realized;
s4: an imaging module formed by an objective lens and a camera is utilized to precisely control the irradiation position and the view field size of the modulated speckle, and the camera is utilized to pre-characterize the speckle information as an input parameter of the subsequent image reconstruction;
s5: the signal collection module focuses the light intensity information after the modulated speckles act on the sample and collects the light intensity information through the point detector, and the image of the sample is reconstructed according to the detected light intensity and speckle information through the compressed sensing reconstruction algorithm.
CN202311081474.9A 2023-08-25 2023-08-25 Cone-shaped optical fiber single-pixel imaging system and method based on compressed sensing Pending CN117288684A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202311081474.9A CN117288684A (en) 2023-08-25 2023-08-25 Cone-shaped optical fiber single-pixel imaging system and method based on compressed sensing

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202311081474.9A CN117288684A (en) 2023-08-25 2023-08-25 Cone-shaped optical fiber single-pixel imaging system and method based on compressed sensing

Publications (1)

Publication Number Publication Date
CN117288684A true CN117288684A (en) 2023-12-26

Family

ID=89257899

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202311081474.9A Pending CN117288684A (en) 2023-08-25 2023-08-25 Cone-shaped optical fiber single-pixel imaging system and method based on compressed sensing

Country Status (1)

Country Link
CN (1) CN117288684A (en)

Similar Documents

Publication Publication Date Title
US9871948B2 (en) Methods and apparatus for imaging with multimode optical fibers
US9885859B2 (en) Structured illumination microscopy apparatus and method
CN103926225B (en) A kind of fluorescent emission differential microscopic method based on evanescent wave illumination and device
CN106767400A (en) Structure detection confocal microscopic imaging method and device based on spatial light modulator
CN101339129A (en) Method and device for variable field of view scanning microscope based on fixed optical path system
CN110118726A (en) A kind of method and apparatus of parallel detecting fluorescent emission difference micro-imaging
CN113049587B (en) High resolution and high imaging speed synthetic aperture phase microscopy system and method
CN103823353B (en) Based on the sub-wavelength super-resolution digital holographic imaging systems of microsphere
CN103954598B (en) A kind of axial high-precision locating method based on evanescent wave illumination and device
CN110109239B (en) Light sheet illumination microscopic imaging method and system for simultaneous multilayer imaging
CN110824681B (en) A scanning-free super-resolution optical three-dimensional microscopy imaging method
CN111024659A (en) A method and device for multi-image reconstruction microscopy based on parallel detection
US20130250088A1 (en) Multi-color confocal microscope and imaging methods
CN109211855A (en) Multiple beam multi-photon microscopic imaging device
CN105043988A (en) Single-point deconvolution microscopic system and imaging method based on scanning galvanometers
CN101122774A (en) Acquisition device of high resolution digital hologram
CN104677865A (en) Microscopic analyzing device
CN102525411A (en) Fluorescent endoscopic imaging method and system
CN208580026U (en) Optical 3D Imaging System
CN220709036U (en) An arbitrary curved surface three-dimensional addressing scanning super-resolution microscopy imaging system
CN117288684A (en) Cone-shaped optical fiber single-pixel imaging system and method based on compressed sensing
CN118641522A (en) A method for interferometric differential super-resolution optical imaging
CN102551661B (en) Fluorescence spectrum endoscopic imaging method and system
US8169695B2 (en) Optical sub-wavelength super resolution imaging system producing nanometric spatial resolution of a scanned subject
CN109883955B (en) Apparatus and method for obtaining optimal structure detection function of structure detection microscope imaging system

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