WO2011106905A1 - 一种可空间编码的并行激发系统及方法 - Google Patents
一种可空间编码的并行激发系统及方法 Download PDFInfo
- Publication number
- WO2011106905A1 WO2011106905A1 PCT/CN2010/000254 CN2010000254W WO2011106905A1 WO 2011106905 A1 WO2011106905 A1 WO 2011106905A1 CN 2010000254 W CN2010000254 W CN 2010000254W WO 2011106905 A1 WO2011106905 A1 WO 2011106905A1
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- Prior art keywords
- excitation
- point
- control module
- parallel
- excitation light
- Prior art date
Links
- 230000005284 excitation Effects 0.000 title claims abstract description 158
- 238000000034 method Methods 0.000 title claims abstract description 16
- 230000003287 optical effect Effects 0.000 claims description 27
- 238000010171 animal model Methods 0.000 claims description 16
- 238000003384 imaging method Methods 0.000 claims description 12
- 239000003550 marker Substances 0.000 claims description 11
- 238000000799 fluorescence microscopy Methods 0.000 claims description 8
- 230000005012 migration Effects 0.000 claims description 5
- 238000013508 migration Methods 0.000 claims description 5
- 238000002474 experimental method Methods 0.000 claims description 4
- 230000008569 process Effects 0.000 claims description 4
- 239000007850 fluorescent dye Substances 0.000 description 3
- 230000002123 temporal effect Effects 0.000 description 3
- 206010028980 Neoplasm Diseases 0.000 description 1
- 230000002159 abnormal effect Effects 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 230000031018 biological processes and functions Effects 0.000 description 1
- 230000001413 cellular effect Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000003745 diagnosis Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 201000010099 disease Diseases 0.000 description 1
- 208000037265 diseases, disorders, signs and symptoms Diseases 0.000 description 1
- 238000009509 drug development Methods 0.000 description 1
- 238000002073 fluorescence micrograph Methods 0.000 description 1
- 230000005865 ionizing radiation Effects 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
- 238000000844 transformation Methods 0.000 description 1
- 230000000007 visual effect Effects 0.000 description 1
Classifications
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
- G01D5/32—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
- G01D5/34—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
- G01D5/347—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells using displacement encoding scales
- G01D5/34707—Scales; Discs, e.g. fixation, fabrication, compensation
- G01D5/34715—Scale reading or illumination devices
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/251—Colorimeters; Construction thereof
- G01N21/253—Colorimeters; Construction thereof for batch operation, i.e. multisample apparatus
Definitions
- This invention relates to optical molecular imaging techniques, and more particularly to a spatially encoded parallel excitation system and method for exciting fluorescence imaging.
- Fluorescent molecular imaging technology is an emerging molecular imaging technology that has developed rapidly in recent years. It has broad application prospects in the fields of tumor detection, drug development and disease diagnosis.
- the technique of exciting fluorescent molecular imaging is to label a specific molecule or cell with a fluorescent label, and when the fluorescent label is irradiated with excitation light of a specific wavelength band, the fluorescent label is excited to emit fluorescence. After scattering and absorption by the tissue, part of the fluorescence reaches the surface of the imaged object.
- a certain device to detect the intensity of the generated fluorescence, a distribution image of the fluorescence optical properties inside the tissue can be obtained, so that normal or abnormal can be obtained at the molecular and cellular levels.
- the spatial and temporal visual description of the biological process is a highly sensitive, non-ionizing radiation, non-invasive and low-cost imaging modality.
- the fluorescence imaging can only obtain the local fluorescence information near the position where the excitation light source can be irradiated, and the fluorescent marker in the far distance from the excitation light source cannot be excited or excited. Weak, this leads to incomplete and inaccurate information on the acquired fluorescence image.
- the fluorescence information of different parts can be obtained by continuously changing the position of the excitation light source several times, this greatly increases the structural complexity of the imaging system, and the imaging time is also multiplied. In practical applications, it is often necessary to observe various fluorescent signals with different temporal and spatial distribution characteristics, especially for some fast-changing fluorescent signals.
- the traditional single-point source excitation method cannot meet the demand.
- a spatially encoded parallel excitation system characterized in that it comprises a parallel excitation array and a spatial coding control system arranged by a plurality of single-point excitation light sources;
- the space coding control system includes a microcontroller, a driving module, a switch control module, an output optical power control module, and an excitation time control module; wherein the switch control module controls opening or closing of each of the single-point excitation light sources;
- Optical power control module Controlling an output optical power of each of the single-point excitation light sources;
- the excitation time control module controls a time during which each of the single-point excitation light sources operates; the switch control module, the output optical power control module, and the excitation time control module
- the micro-controller performs parameter setting; the micro-controller sets the working state of each single-point excitation light source in the parallel excitation array by the driving module according to the corresponding parameter setting, and realizes the spatial coding control system Spatial coding of the parallel ex
- the single point excitation source is a high power LED or a laser diode.
- the parallel excitation array is an array of rectangles, circles, sectors or other shapes.
- a spatially encoded parallel excitation method based on the above system, comprising the following steps: (1) determining a required parallel excitation mode according to specific experimental conditions such as experimental purpose, experimental animal and fluorescent marker; (2) determining A good parallel excitation mode input spatial coding control system sets the working state of each single-point excitation light source through each module in the spatial coding control system to realize spatial coding of the parallel excitation array; (3) in the spatially encoded parallel excitation array Fluorescence imaging was performed under excitation.
- the content of the parallel excitation mode includes the number, distribution, and output optical power, excitation time, and excitation order of the single-point excitation light source required for the experiment, and specifically includes the following four modes: When it is required to integrally image the whole body distribution of the fluorescent marker in the experimental animal, the plurality of the single-point excitation light sources are selected to be simultaneously excited, and the number of the single-point excitation light source is determined by the volume of the experimental animal. The output optical power and excitation time of the single-point excitation source are determined according to the specific experimental requirements. 2 When local imaging of the distribution of fluorescent markers in a small area of the experimental animal is required, the selection is based on the location of the region.
- Exciting is performed by using one of the single-point excitation light sources, and the output optical power and excitation time of the single-point excitation light source are determined according to specific experimental requirements; 3 when it is required to track the dynamic process of fluorescent marker migration in the experimental animal, select Exciting sequentially using a plurality of said single-point excitation sources, The excitation time of the single-point excitation light source is set to coincide with the passage time of the fluorescent marker at the point, and the output optical power is determined according to specific experimental requirements; 4, according to actual needs, the selection is performed by point-by-point scanning excitation, and each row/column is sequentially excited, Interlaced/column excitation or two rows/column alternate excitation modes.
- the invention adopts the above technical solution, and has the following advantages compared with the prior art - the invention adopts the spatial coding parallel excitation technology, and can set the working state of each single-point excitation light source in the point light source array according to actual needs, It can be used for the overall observation of the temporal and spatial characteristics of the distribution of fluorescent markers in experimental animals, as well as the close-up observation of the distribution of fluorescent markers in local regions, and can also be used to dynamically track the migration process of specific fluorescent markers. Wait.
- the spatially encoded parallel excitation method designed by the invention has the advantages of flexibility, high efficiency, convenient use, high imaging time and high spatial resolution, and wide application range.
- FIG. 1 is a block diagram of the structure of the present invention
- FIG. 2 is a schematic structural view of a parallel excitation array in the present invention
- the present invention includes a parallel excitation array 1 and a spatial encoding control system 2.
- the parallel excitation array 1 includes a plurality of single-point excitation light sources 11 (marked as . in the figure, indicating the row where the single-point excitation light source 1 1 is located, indicating the column of the single-point excitation light source 11), and several single-point excitation light sources 1 1 Arranged into an array of > ⁇ « columns, the spacing between two adjacent columns is, the spacing between two adjacent rows is, wherein the specific values of n, d, are determined according to actual needs.
- the spatial coding control system 2 includes a microcontroller 21, a drive module 22, a switch control module 23, an output optical power control module 24, and an excitation time control module 25.
- the switch control module 23 controls the opening or closing of each single-point excitation light source 11; the output optical power control module 24 controls the output optical power of each single-point excitation light source 11; and the excitation time control module 25 controls the operation of each single-point excitation light source 11 time.
- the switch control module 23, the output optical power control module 24, and the excitation time control module 25 parameterize the microcontroller 21.
- the microcontroller 21 sets the working state of each single-point excitation light source 11 in the parallel excitation array 2 through the driving module 22 according to the corresponding parameter setting, thereby realizing the spatial encoding of the parallel excitation array 1 by the spatial coding control system 2.
- the single-point excitation light source 11 may be a high-power LED (light-emitting secondary light) or a laser diode.
- a plurality of single-point excitation light sources 11 may also be arranged in an array of circular, fan-shaped or other shapes according to different requirements.
- the content of the parallel excitation mode includes the number, distribution, and output optical power, excitation time, and excitation order of the single-point excitation light source 11 required for the experiment, and specifically includes the following four modes - 1
- it is necessary to perform an overall imaging of the whole body distribution of the fluorescent marker in the experimental animal it is possible to selectively use the ⁇ S , , ⁇ _ / single-point excitation light source 11 simultaneously.
- the specific value of _ / is determined by the size of the experimental animal, and the output optical power and excitation time of each single-point excitation light source 11 are determined according to specific experimental requirements;
- a single point excitation source 11 can be selected for excitation.
- the specific value is determined by the location of the region, and the output optical power and excitation time of the single-point excitation source 11 are determined according to specific experimental requirements;
- the content of the parallel excitation mode is input to the spatial coding control system 2, and the working states of the single-point excitation light sources 11 are set by the respective modules in the spatial coding control system 2 (
- the spatial encoding of the parallel excitation array 1 is achieved by including whether the single-point excitation light source 11 is turned on, its output optical power and excitation time, and the excitation order between the plurality of single-point excitation light sources 11.
- Fluorescence imaging was performed under excitation of a spatially encoded parallel excitation array 1 .
- the working mode of the parallel excitation array 1 can be adjusted by the spatial coding control system 2 according to the new experimental requirements, and a new fluorescence imaging experiment can be performed.
Description
Claims
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CA2782964A CA2782964C (en) | 2010-03-02 | 2010-03-02 | Parallel excitation system capable of spatial encoding and method thereof |
CN201080000866.2A CN102036602B (zh) | 2010-03-02 | 2010-03-02 | 一种可空间编码的并行激发系统及方法 |
PCT/CN2010/000254 WO2011106905A1 (zh) | 2010-03-02 | 2010-03-02 | 一种可空间编码的并行激发系统及方法 |
Applications Claiming Priority (1)
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PCT/CN2010/000254 WO2011106905A1 (zh) | 2010-03-02 | 2010-03-02 | 一种可空间编码的并行激发系统及方法 |
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WO2011106905A1 true WO2011106905A1 (zh) | 2011-09-09 |
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PCT/CN2010/000254 WO2011106905A1 (zh) | 2010-03-02 | 2010-03-02 | 一种可空间编码的并行激发系统及方法 |
Country Status (3)
Country | Link |
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CN (1) | CN102036602B (zh) |
CA (1) | CA2782964C (zh) |
WO (1) | WO2011106905A1 (zh) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPWO2014069647A1 (ja) * | 2012-11-05 | 2016-09-08 | 全薬工業株式会社 | 抗体又は抗体組成物の製造方法 |
Families Citing this family (1)
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CN113092411B (zh) * | 2018-10-12 | 2022-11-11 | 上海禾赛科技有限公司 | 一种基于激光器阵列实现接收光强自稳定的装置及方法 |
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JP2006000666A (ja) * | 1996-03-19 | 2006-01-05 | Matsushita Electric Ind Co Ltd | 蛍光診断治療装置 |
US20060249689A1 (en) * | 2005-03-18 | 2006-11-09 | Norbert Eustergerling | Apparatus for generating 3D fluorscence of luminescence |
CN100407985C (zh) * | 2002-07-18 | 2008-08-06 | 莫纳基技术公司 | 高分辨率光纤荧光成像的方法和装置 |
WO2009009178A2 (en) * | 2007-04-06 | 2009-01-15 | The General Hospital Corporation | Systems and methods for optical imaging using early arriving photons |
CN101396262A (zh) * | 2008-10-31 | 2009-04-01 | 清华大学 | 一种基于线性关系的荧光分子断层成像重建方法 |
CN101461706A (zh) * | 2007-12-19 | 2009-06-24 | 坎通斯比特阿劳股份有限公司 | 用于分析和处理荧光图像的方法 |
CN101539518A (zh) * | 2008-03-20 | 2009-09-23 | 中国科学院自动化研究所 | 一种用于自发荧光成像的空间加权的有限元重建方法 |
-
2010
- 2010-03-02 WO PCT/CN2010/000254 patent/WO2011106905A1/zh active Application Filing
- 2010-03-02 CA CA2782964A patent/CA2782964C/en not_active Expired - Fee Related
- 2010-03-02 CN CN201080000866.2A patent/CN102036602B/zh not_active Expired - Fee Related
Patent Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
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JP2006000666A (ja) * | 1996-03-19 | 2006-01-05 | Matsushita Electric Ind Co Ltd | 蛍光診断治療装置 |
CN100407985C (zh) * | 2002-07-18 | 2008-08-06 | 莫纳基技术公司 | 高分辨率光纤荧光成像的方法和装置 |
US20060249689A1 (en) * | 2005-03-18 | 2006-11-09 | Norbert Eustergerling | Apparatus for generating 3D fluorscence of luminescence |
WO2009009178A2 (en) * | 2007-04-06 | 2009-01-15 | The General Hospital Corporation | Systems and methods for optical imaging using early arriving photons |
CN101461706A (zh) * | 2007-12-19 | 2009-06-24 | 坎通斯比特阿劳股份有限公司 | 用于分析和处理荧光图像的方法 |
CN101539518A (zh) * | 2008-03-20 | 2009-09-23 | 中国科学院自动化研究所 | 一种用于自发荧光成像的空间加权的有限元重建方法 |
CN101396262A (zh) * | 2008-10-31 | 2009-04-01 | 清华大学 | 一种基于线性关系的荧光分子断层成像重建方法 |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
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JPWO2014069647A1 (ja) * | 2012-11-05 | 2016-09-08 | 全薬工業株式会社 | 抗体又は抗体組成物の製造方法 |
Also Published As
Publication number | Publication date |
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CA2782964C (en) | 2016-01-19 |
CA2782964A1 (en) | 2011-09-09 |
CN102036602B (zh) | 2012-09-05 |
CN102036602A (zh) | 2011-04-27 |
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