• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The imaging system (20) includes a receiving medium (26) configured to receive a sample (24), a light source (30) configured to emit a light beam (50) of illumination of the sample (24). ) in a direction of illumination (Z), the light source (30) having a diode (52) and a diaphragm (54), the diaphragm (54) being disposed between the diode (52) and the receiving medium ( 26) in the illumination direction (Z), and a matrix photodetector (32) configured to acquire at least one image of the sample (24), each image being formed by radiation transmitted by the illuminated sample (24) and having at least one elementary diffraction pattern, the receiving medium (26) being disposed between the light source (30) and the matrix photodetector (32) in the illumination direction (Z). The system (20) further includes a light diffuser (56) disposed between the diode (52) and the diaphragm (54).
    公开号:FR3028951A1
    申请号:FR1461316
    申请日:2014-11-21
    公开日:2016-05-27
    发明作者:Thomas Bordy
    申请人:Commissariat a lEnergie Atomique CEA；Commissariat a lEnergie Atomique et aux Energies Alternatives CEA；
    IPC主号:
    专利说明:

    [0001] A lensless imaging system comprising a diode, a diaphragm and a diffuser between the diode and the diaphragm The present invention relates to an imaging system without a lens. The imaging system includes a receiving medium configured to receive a sample and a light source configured to emit a sample illumination light beam in a direction of illumination, the light source having a diode and a diaphragm , the diaphragm being disposed between the diode and the receiving medium in the direction of illumination.
    [0002] The imaging system also comprises a matrix photodetector configured to acquire at least one image of the sample, each image being formed by radiation transmitted by the illuminated sample and comprising at least one elementary diffraction pattern, the receiving medium being disposed between the light source and the matrix photodetector in the direction of illumination.
    [0003] The invention relates to imaging without a lens, also called contact imaging, that is to say the acquisition, by the matrix photodetector, of images formed by the radiation transmitted directly by the sample, in the absence a magnification optics arranged between the sample and the matrix photodetector. In this case, the matrix photodetector is also called imaging device without a lens, and capable of forming an image of the sample while being placed at a small distance from it. By short distance is meant a distance of between 100 lm and a few centimeters, preferably less than 1 cm. Document EP 2 122 326 B1 discloses an imaging system of the aforementioned type. The imaging system includes a light source adapted to illuminate a sample and a CCD sensor capable of acquiring at least one image of the illuminated sample. The light source comprises a light-emitting diode with an opening diameter equal to 60 or a wide-area light-emitting diode associated with a diaphragm, also called pinhole, having a diameter equal to 6. diffraction observed then comprise a center and one or more concentric rings arranged around the center. However, the diffraction patterns observed with such an imaging system are not optimal, particularly when the surface of the diode is too large, the diaphragm projects the image of the electrode or electrodes constituting the light emitting diode onto the sensor. Thus, in the absence of sample, the image collected on the sensor is not homogeneous.
    [0004] 3028951 2 This effect occurs in the presence of a sample, which affects the quality of the images obtained. The object of the invention is therefore to provide an imaging system to solve this problem.
    [0005] To this end, the invention relates to an imaging system of the aforementioned type, wherein the system further comprises a light diffuser disposed between the diode and the diaphragm. According to other advantageous aspects of the invention, the imaging system comprises one or more of the following features, taken alone or in any technically possible combination: the diode is a light-emitting diode; the diode is a laser diode, such as a VCSEL laser diode; the light diffuser has a diffusion angle, and the value of the diffusion angle is greater than or equal to 5 °, preferably greater than or equal to 20 °, more preferably greater than or equal to 30 °; the scattering angle satisfies the following equation: Va2 + A2 where A represents the scattering angle of the light scatterer, a represents a divergence angle of the diode, and [3 represents a scattering angle resulting in an output light diffuser; the diode has an angle of divergence, the light diffuser has a scattering angle, and the value of the divergence angle is smaller than the value of the scattering angle; - The light diffuser has a smooth surface and a diffusing surface, and the diffusing surface is disposed away from the diaphragm; The light diffuser is made of a material selected from the group consisting of: a polyester, a polycarbonate and an acrylic material; the diaphragm has a diameter of between 50 μm and 500 μm, preferably substantially equal to 150 μm; the distance between the support and the diaphragm in the direction of illumination is between 1 cm and 30 cm, preferably between 1 cm and 10 cm, more preferably substantially equal to 5 cm; and the distance between the support and the matrix photodetector in the direction of illumination is less than or equal to 1 cm, and preferably less than 5 mm.
    [0006] These features and advantages of the invention will appear on reading the description which will follow, given solely by way of nonlimiting example, and with reference to the appended drawings, in which: FIG. 2 is a very schematic representation of the imaging system of FIG. 1, comprising a light source suitable for illuminating a sample and a matrix photodetector able to establish a diffraction pattern transmitted by the illuminated sample, the light source having a diode, a diaphragm and a light diffuser disposed between the diode and the diaphragm; and FIG. 3 is a view of an area of an image acquired with an imaging system of the state of the art, - Figure 4 is a view of an area of an image acquired with the imaging system of Figures 1 and 2, - Figure 5 is a profile. Intensity of the FIG. 6 is an intensity profile of the region of the image of FIG. 4 along the line VI, FIG. 7 is a view similar to FIG. that of FIG. 5 along line VII; FIG. 8 is a view similar to that of FIG. 6 along line VIII; FIG. 9 is a view of a diffraction pattern acquired with the imaging system of the state of the art, FIG. 10 is a view of a diffraction pattern acquired with the imaging system of FIGS. 1 and 2; FIG. 11 is a profile of intensity of the image of FIG. FIG. 9 along line XI; FIG. 12 is an intensity profile of the image of FIG. 10 along line XII; FIG. 13 is a view of an image acquired with the matrix photodetector of FIG. FIG. 14 is an intensity profile of the image of FIG. 13 along the line XIV, FIGS. 15, 17, 19, 21 are respective views of an image of FIG. image acquired with the imaging system of FIGS. 1 and 2, for different values of a scattering angle of the light diffuser, and FIGS. 16, 18, 20 and 22 are each an intensity profile of FIG. FIGS. 15, 17, 19 and 21, respectively, along the lines XVI, XVIII, XX and respectively XXII.
    [0007] Conventionally, in the present application, the expression "substantially equal to" will express a relationship of equality at plus or minus 10%, preferably at plus or minus 5%. In Figs. 1 and 2, a sample imaging system 24 comprises a receiving medium 26 adapted to receive the sample 24. The imaging system 20 also includes a light source 30 and a matrix photodetector 32 adapted to acquire several successive images of radiation transmitted by the sample 24 illuminated by the light source 30. The imaging system 20 is generally adapted to acquire one or more images of the sample 24 via a imaging methodology without a lens, the matrix photodetector 32 having no magnification optics. The imaging system 20 also comprises an information processing unit 34, visible in FIG. 2, comprising a memory 36 and a processor 38 associated with the memory 36.
    [0008] In addition, the imaging system 20 comprises a device 40 with hinged doors, the doors being painted black, making it possible to isolate the radiation transmitted by the illuminated sample 24 from the external environment. The hinged door device 40 allows, when the swing doors are closed, the technician to operate then in ambient light, without disturbing the measurements made inside the imaging system. The imaging system 20 also comprises a heat sink 42 and a fan 44 for regulating the temperature of the matrix photodetector 32, in particular to cool it in case of overheating. These elements are optional. The sample 24 comprises particles 45, called diffracting particles in the following description, each particle 45 being able to generate diffracted waves during the illumination of the sample 24. The sample 24 is, for example, a liquid, such as a body fluid that has previously been removed from a patient, the sampling step not being within the scope of the invention. Sample 24 comprises for example cerebrospinal fluid or blood. The receiving medium 26 is disposed between the light source 30 and the matrix photodetector 32, and is substantially perpendicular to a vertical direction Z corresponding to the illumination direction of the sample 24 by the light source 30, as shown in FIG. Figure 2.
    [0009] The receiving support 26 comprises a transparent plate 48, made for example of glass. In this example, the receiving medium 26 is deposited at the bottom of a Petri dish 46. The Petri dish 46 here has a sample containment function 24, and is optional. It is adapted to be deposited directly on the matrix photodetector 32. The Petri dish 46 additionally comprises a cover 49 in order to protect the sample 24.
    [0010] The light source 30 is adapted to emit a light beam 50 in the vertical direction Z to illuminate the sample 24 having the diffracting particles 45. The light source 30 is disposed at a first distance D1 of the transparent plate 48 in the direction of illumination, corresponding in the example of Figures 1 and 2 to the vertical direction Z. The first distance D1 preferably has a value between 1 cm and 30 cm, preferably between 1 cm and 20 cm, preferably between 1 cm and 10 cm, more preferably substantially equal to 5 cm. The first distance D1 corresponds to the distance between the light source 30 and the receiving medium 26 in the direction of illumination, and more precisely at the distance between the diaphragm 54 and the blade 48 in this direction of illumination. The light source 30 is preferably spatially coherent and preferably monochromatic. The term monochromatic designates a spectral width less than 80 nm, preferably less than 50 nm at half height. The light source 30 includes a diode 52, also called LED (Light Emetting Diode), and a diaphragm 54, as schematically shown in Fig. 2. The diaphragm 54 is also called pinhole (of the English pinhole). According to the invention, the light source 30 further comprises a light diffuser 56 disposed between the diode 52 and the diaphragm 54 in the direction of illumination.
    [0011] The matrix photodetector 32 is adapted to acquire successive images of the radiation transmitted by the sample 24 containing the diffracting particles 45, illuminated by the light beam 50. By transmitted radiation is meant the radiation passing through the sample 24 so that the matrix photodetector 32 and the light source 30 are situated on either side of the sample 24 comprising the diffracting particles 45. The matrix photodetector 32 is a two-dimensional image sensor, namely in a plane substantially perpendicular to the vertical axis Z. The matrix photodetector 32 is a pixelated image sensor, for example a CMOS (English Complementary Metal Oxide Semiconductor) sensor. In a variant, the matrix photodetector 32 is a CCD (Charge Coupled Device) sensor.
    [0012] The matrix photodetector 32 comprises a plurality of pixels, not shown, each having dimensions less than or equal to 10 μm, and preferably less than 5 μm, and even more preferably less than 2 μm. The matrix photodetector 32 may further comprise microlenses, not shown, each microlens being disposed above a corresponding pixel. Such microlenses are integrated in the sensor and make it possible to improve the collection efficiency, without however forming a magnification optics arranged between the receiving medium 26 and the photodetector 32. The images acquired by the matrix photodetector 32 are formed by the 10 radiation transmitted directly by the illuminated sample 24, in the absence of magnification optics disposed between the receiving medium 26 and the matrix photodetector 32. The photodetector 32 is also called imaging device without a lens, and is able to form an image of the liquid 24, while being placed at a short distance from the latter. By short distance is meant a distance of less than a few centimeters, preferably less than 1 cm. The photodetector 32 is disposed at a second distance D2 from the transparent plate 48 in the direction of illumination, and the second distance D2 is then less than a few centimeters, preferably less than 1 cm. The fact of favoring a low value for the second distance D2, that is to say a small distance between the matrix photodetector 30 and the receiving medium 26, 20 makes it possible to limit the phenomena of interference between different diffraction patterns when sample 24 is illuminated. The matrix photodetector 32 is then able to make an image of at least one elementary diffraction pattern 60 transmitted by the sample 24, each elementary diffraction pattern 60 corresponding to waves diffracted by a diffractive particle 45, during the illumination of the sample 24. Thus, the matrix photodetector 32 makes it possible to obtain an image 11 comprising one or more elementary diffraction patterns 60. Each image acquired ln by the matrix photodetector 32 comprises a plurality of pixels In (x, y), each being marked x and x on the y-axis in the image 30 and the matrix photodetector 32 is adapted to measure the intensity 1 (x, y) of each pixel. The memory 36 is able to store a software 70 for processing one or more images of the sample 24. The processor 38 is adapted to execute the processing software 70. The diffractive particles 45 are, for example, biological particles, that is, cells (especially blood cells, e.g., white blood cells or red blood cells), bacteria or bacterial colonies, or cell aggregates. As a variant, the diffractive particles 45 are microbeads, dust, pollen or surface roughness of the sample 24.
    [0013] Those skilled in the art will then understand that the imaging system 20 according to the invention is a lensless imaging system, adapted to acquire any image comprising one or more elementary diffraction patterns 60, each corresponding elementary diffraction pattern 60 to waves diffracted by a particle 45 during illumination of the sample 24, regardless of the type of particle 45, and in general regardless of the sample type 24. The diffracting particles 45 generally have a smaller diameter at 100 iim. The diameter of the diffracting particles 45 is, for example, between 1 μm and 100 μm. Cells, such as white blood cells and red blood cells, have a diameter of the order of 10 microns.
    [0014] Diode 52 has an angle of divergence a. By divergence angle is meant the half angle of the emission cone of the diode 52. The diode 52 is, for example, a light emitting diode. The light-emitting diode for example has a wavelength substantially equal to 525 nm.
    [0015] Alternatively, the diode 52 is a laser diode, such as a Vertical Cavity Surface Emitting Laser (VCSEL) type laser diode. The diaphragm 54 has, for example, a diameter of between 50 μm and 500 μm, preferably substantially equal to 150 μm. This makes it possible to increase the spatial coherence of the light radiation.
    [0016] The light diffuser 56 has an angle of diffusion A. The value of the diffusion angle A is, for example, greater than or equal to 20 °, preferably greater than or equal to 30 °, more preferably greater than or equal to 40 °. Diffusion angle A satisfies the following equation: λ Va2 ± A2 (1) where A represents the scattering angle of the light diffuser 56, a represents the divergence angle of the diode 52, and [3 represents a scattering angle resulting from the output of the light diffuser 56. The value of the divergence angle a is preferably smaller than the value of the diffusion angle A.
    [0017] The light diffuser 56 has, in the direction of illumination, a thickness E of value between 100 μm and 1 mm, preferably between 500 μm and 2 mm. The light diffuser 56 is for example in the form of a thin and flexible film, and its thickness is then typically less than or equal to 1.5 mm, for example between 0.5 mm and 1 mm. In a variant, the light diffuser 56 is in the form of a rigid substrate, and its thickness is then typically greater than or equal to 0.5 mm, for example between 2 mm and 3 mm. The light diffuser 56 is made of a material selected from the group consisting of: a polyester, a polycarbonate and an acrylic material.
    [0018] The light diffuser 56 is for example arranged in contact with the diaphragm 54, more precisely in contact with the face of the diaphragm 54 which is directed towards the diode 52, that is to say in contact with the upper face of the diaphragm 54 in the example of FIGS. 1 and 2. In a variant, the light diffuser 56 is disposed in contact with the diode 52, more precisely in contact with the face of the diode 52 which is directed towards the diaphragm 54; that is to say in contact with the lower face of the diode 52 in the example of Figures 1 and 2. In another variant, the light diffuser 56 is disposed away from the diode 52 and the diaphragm 54. According to a In one embodiment, the light diffuser 56 has a diffusing layer 56A deposited on a substrate 56B, the latter acting as a support for the diffusing layer 56A. The substrate 56B forms a smooth surface, and the diffusing layer 56A forms a diffusing surface. In such an embodiment, it has been found that the diffusing layer 56A is preferably arranged at a distance from the diaphragm 54, and for example at a distance greater than 50 μm or more than 100 μm from the diaphragm 54 in the direction In other words, the diffusing surface is preferably disposed away from the diaphragm 54. Each elemental diffraction pattern 60 comprises a central zone 80, also called a center, the intensity of which is substantially homogeneous. central 80 being surrounded by concentric rings 82, 84, 86, 88 whose intensity is alternately low (dark rings) and high (clear rings), as shown in FIGS. 9 and 10. The rings 82, 84, 86 , 88 correspond respectively to a first light ring, a second light ring, a third light ring and a fourth light ring. The processing software 70 forms means for processing the acquired image (s) of the sample 24.
    [0019] As a variant, the processing means 70 are made in the form of programmable logic components or in the form of dedicated integrated circuits.
    [0020] The processing software 70 is, for example, adapted to identify, from the acquired images ln, In + 1, moving elementary diffraction figures 60, and to count moving particles 45 within the sample 24, from the identified mobile elementary diffraction patterns.
    [0021] In addition or alternatively, the processing software 70 is adapted to characterize each identified elementary diffraction pattern 60, that is, to determine one or more criteria for each of these figures. Such a criterion is, for example, a ratio R between the maximum intensity and the median intensity (or average intensity) of a region of interest of said diffraction figure.
    [0022] The processing software 70 is then able to sort the detected elementary diffraction patterns 60 according to at least two distinct categories according to the chosen characterization criterion, in order to classify the particles corresponding to the elementary diffraction patterns detected according to distinct classes. The classification of said diffraction pattern 60 is, for example, performed by comparing the calculated ratio R with at least one predetermined threshold. As a variant, the processing software 70 is adapted to reconstruct the optical properties of the sample 24, in particular the absorption or the phase retardation, from an image acquired by the matrix photodetector 32. In a variant, the software of FIG. Treatment 70 is adapted to characterize a variation in the speed of the particles 45 contained in the sample 24 or to characterize an agglomeration of said particles 45, especially when the sample 24 is a liquid sample containing blood, and the particles 45 are blood particles. Those skilled in the art will then understand that the imaging system 20 according to the invention is suitable for any type of application using an imaging system without a lens, the imaging system 20 according to the invention making it possible to to improve the quality of the images acquired by the matrix photodetector 32, as will now be described with reference to FIGS. 3 to 22, whatever the type of application. FIG. 3 shows an area 100 of an image acquired with an imaging system of the state of the art, that is to say with an imaging system having no light diffuser disposed between the diode and the diaphragm in the direction of illumination. The zone 100 comprises several elementary diffraction patterns 60. FIG. 4 represents a zone 200 of an image acquired with the imaging system 20 according to the invention, comprising the light diffuser 56 disposed between the diode 52 and the diaphragm 54 according to the direction of illumination. The zone 200 also comprises several elementary diffraction figures 60.
    [0023] The zone 100 and the zone 200 each correspond to the same portion of the illuminated sample 24, as evidenced by the presence of the black disk near the center of each of the zones 100 and 200. It can be seen that the acquired image With the imaging system 20 according to the invention is much more homogeneous than that acquired with the imaging system of the state of the art. Indeed, the zone 100 has a darkening of its periphery, especially with the dark corners on the left of Figure 3, with a similar rendering vignetting, while the 200 zone does not have such a darkening of its periphery. Furthermore, the zone 100 has a darkening in its central part, this darkening being noticeable on the zone 200. This is confirmed by FIGS. 5 to 8 which each represent an intensity profile along a respective line V to VIII Figures 3 and 4. Each profile is an intensity profile expressed in gray level according to a distance expressed in iim. The profiles corresponding to the imaging system of the state of the art are the profiles 110 and 120, visible in FIGS. 5 and 7, respectively along the lines V and VII of FIG. 3. The profile 110 along the line V is also called vertical profile, and the profile 120 along the line VII is also called horizontal profile. The profiles corresponding to the imaging system 20 according to the invention are the profiles 210 and 220, visible in FIGS. 6 and 8, respectively along the lines VI and VIII of FIG. 4. In a similar way, the profile 210 according to FIG. Line VI is also called vertical profile, and profile 220 along line VIII is also called horizontal profile. Those skilled in the art will then observe that the profiles 210 and 220 obtained with the imaging system 20 according to the invention each have, apart from a few punctual peaks, a small variation of the intensity in gray level, the average value being at Each time close to the value 50. In contrast, the profiles 110 and 120, obtained with the imaging system of the stage of the technique, have, apart from a few punctual peaks, a significant variation in the intensity, this varies between about 50 and 130 for the vertical profile 110 and between about 20 and 120 for the vertical profile 120. In addition, the imaging system 20 according to the invention makes it possible to have a better resolution of the diffraction rings 82 , 84, 86, 88, as will now be explained with reference to FIGS. 9 to 12. Indeed, the diffraction pattern shown in FIG. 10 has a higher contrast than that shown in FIG. 9. In addition, the image system 20 of the invention is more robust with respect to an offset of the position of the light source 30 with respect to the central axis of the diaphragm 54. The insertion of the diffuser 56 between the light source 30 and the diaphragm 54 makes the imaging system 20 more tolerant of such an offset.
    [0024] FIG. 9 represents an area of interest 140 of an image acquired with the imaging system of the state of the art, this area of interest 140 comprising a corresponding elementary diffraction figure 60 with its center 80 and its rings 82, 84, 86. FIG. 10 represents a similar zone of interest 240 of an image acquired with the imaging system 20 according to the invention, this zone of interest 240 also comprising an elementary diffraction pattern 60 with its center 80 and its rings 82, 84, 86, 88. A visual comparison of FIGS. 9 and 10 then makes it possible to observe a much better visibility of the diffraction rings 82, 84, 86, 88 on the image acquired with The imaging system 20 according to the invention than that acquired with the imaging system of the state of the art. In other words, the rings 82, 84, 86, 88 stand out more clearly, or have a better resolution, on the image acquired via the imaging system 20 according to the invention. This visual perception is confirmed by FIGS. 11 and 12 respectively representing a vertical profile 150 along the line XI of FIG. 9, obtained with the imaging system of the state of the art, and a vertical profile 250 along the line XII of Figure 10, obtained with the imaging system 20 according to the invention. Comparison of the vertical profiles 150 and 250 then clearly shows that the second light ring 84, as well as the following light rings 86, 88, correspond to distinct peaks of intensity on the vertical profile 250 obtained with the imaging system. 20 according to the invention only on the vertical profile 150 obtained with the imaging system of the state of the art. The imaging system 20 according to the invention then makes it possible to reduce or even avoid a loss of resolution on the rings 82, 84, 86, 88 of the elementary diffraction figures 60.
    [0025] As previously described, the invention relates to any light diffuser 56 disposed between the diode 52 and the diaphragm 54 in the direction of illumination. The inventors have furthermore found that the results obtained are even better for certain values of the diffusion angle A of the light diffuser 56, as will be described hereinafter with reference to FIGS. 13 to 22.
    [0026] Fig. 13 shows an image 300 acquired with the prior art imaging system, and Fig. 14 shows the corresponding vertical intensity profile 305 along the line XIV. FIGS. 15, 17, 19 and 21 each represent an image 400, 410, 430, 440 acquired by the imaging system 20 according to the invention, for increasing values of the diffusion angle A, the corresponding FIG. at a value substantially equal to 5 ° of the diffusion angle A, FIG. 17 corresponding to a value substantially equal to 10 ° of said diffusion angle A, FIG. 19 corresponding to a value substantially equal to 40 ° of said angle A, and FIG. 21 corresponding to a value substantially equal to 60 ° of said diffusion angle A. FIGS. 16, 18, 20 and 22 represent the vertical profiles of intensity 405, 415, 435, 445 respectively corresponding to the lines XVI, XVIII, XX and XXII of Figures 15, 17, 19 and 21. In the example of Figures 13, 15, 17, 19 and 21, the transparent plate 48 has points each defining a pattern. These points appear in FIGS. 13, 15, 17, 19 and 21, as well as in FIGS. 3 and 4. It can be seen that the darkening of the periphery of the acquired image is most marked with the system of FIG. imaging of the state of the art corresponding to the image 300, and that the only addition of the light diffuser 56, even with a low value of its diffusion angle A as in the case of the image 400 with an angle of diffusion A substantially equal to 5 °, reduces this darkening of the periphery of the acquired image. This is also observed via the profiles 405, 415, 435 and 445 obtained with the imaging system 20 according to the invention, which have less intensity variations than for the profile 305 obtained with the imaging system of FIG. the state of the art. It should further be noted that the entire image acquired has an almost uniform intensity from the moment when the value of the diffusion angle A is greater than or equal to 20 °, in particular greater than or equal to 30 °, as illustrated by the profiles 435, and 445 respectively, having an intensity value substantially equal to 100 in gray level, and 150 respectively in gray level. It is thus conceived that the imaging system 20 according to the invention makes it possible to improve the image or images acquired by the matrix photodetector 32, in particular to have diffraction patterns 60 with diffraction rings 82, 84, 86 , 88 more visible.
    权利要求:
    Claims (11)
    [0001]
    An imaging system (20) comprising: - a receiving medium (26) configured to receive a sample (24); - a light source (30) configured to emit a light beam (50) of illumination of the sample (24) in an illumination direction (Z), the light source (30) having a diode (52) and a diaphragm (54), the diaphragm (54) being disposed between the diode (52) and the receiving medium (26) in the illumination direction (Z); - a matrix photodetector (32) configured to acquire at least one image of the sample (24), each image being formed by radiation transmitted by the illuminated sample (24) having at least one elementary diffraction pattern (60), the receiving medium (26) being disposed between the light source (30) and the matrix photodetector (32) in the direction of illumination (Z ), characterized in that the system (20) further comprises a light diffuser (56) disposed between the diode (52) and the diaphragm (54).
    [0002]
    The system (20) of claim 1, wherein the diode (52) is a light emitting diode.
    [0003]
    The system (20) of claim 1, wherein the diode (52) is a laser diode, such as a VCSEL laser diode.
    [0004]
    The system (20) according to any one of the preceding claims, wherein the light diffuser (56) has a scattering angle (A), and the scattering angle value (A) is greater than or equal to at 5 °, preferably greater than or equal to 20 °, more preferably greater than or equal to 30 °.
    [0005]
    5. System (20) according to claim 4, wherein the diffusion angle (A) satisfies the following equation: / 3 Va2 + A2 where A represents the diffusion angle of the light diffuser (56), a represents a divergence angle of the diode (52), and [3] represents a diffusion angle resulting from the output of the light diffuser (56). 3028951 14
    [0006]
    The system (20) according to any of the preceding claims, wherein the diode (52) has a divergence angle (a), the light diffuser (56) has a scattering angle (A), and the value of the angle of divergence (a) is less than the value of the scattering angle (A). 5
    [0007]
    The system (20) of any one of the preceding claims, wherein the light diffuser (56) has a smooth surface (56B) and a diffusing surface (56A), and the diffusing surface (56A) is disposed at the gap of the diaphragm (54). 10
    [0008]
    The system (20) of any preceding claim, wherein the light diffuser (56) is made of a material selected from the group consisting of: polyester, polycarbonate and acrylic material.
    [0009]
    9. A system (20) according to any one of the preceding claims, wherein the diaphragm (54) has a diameter of between 50 μm and 500 μm, preferably substantially 150 μm.
    [0010]
    10.- System (20) according to any one of the preceding claims, wherein the distance (D1) between the support (26) and the diaphragm (54) in the direction of illumination (Z) is between 1 cm and 30 cm, preferably between 1 cm and 10 cm, more preferably substantially equal to 5 cm.
    [0011]
    11. A system (20) according to any one of the preceding claims, wherein the distance (D2) between the support (26) and the matrix photodetector (32) in the direction of illumination (Z) is less than or equal to at 1 cm, and preferably less than 5 mm.
    类似技术:
    公开号 | 公开日 | 专利标题
    EP3221688B1|2019-02-20|Lens-free imaging system comprising a diode, a diaphragm and a diffuser between the diode and the diaphragm
    EP3137874B1|2019-04-10|Method for diagnosing meningitis
    EP2556164B1|2018-05-30|Method for detecting clusters of biological particles
    EP2912436B1|2020-10-21|Method for observing biological species
    WO2018138223A1|2018-08-02|Optical detector of particles
    EP2356429A1|2011-08-17|Device for analyzing a polyphase mixture via a light beam backscattered by said mixture
    EP2914952B1|2021-01-06|Device for acquiring an image of a sample, comprising a facility for regulating the heating of a support for receiving the sample, and associated imaging system
    EP2872871A1|2015-05-20|Method and system for reconstructing optical properties of diffracting objects bathed in a liquid medium
    EP3559635B1|2021-11-03|Device and method for observing the radiation backscattered by an object
    EP3270232A1|2018-01-17|Device for observing a sample
    EP3559636A1|2019-10-30|Device and method for observing the radiation backscattered by an object
    CA2701151A1|2009-04-30|Imaging system with wavefront modification and method of increasing the depth of field of an imaging system
    WO2016120276A1|2016-08-04|Methods and devices for detecting surface contamination by particles in free air
    EP3230713B1|2020-07-29|Method for obtaining an image of a sample, and associated lens-free imaging system
    EP3213049B1|2021-08-18|Method and system for estimating a concentration of a species in a culture medium by lensless imaging
    WO2018109350A1|2018-06-21|Protection device used in a lensless imaging detection system and lensless imaging detection system using said device
    EP3598102A1|2020-01-22|Optical particle sensor
    WO2021009465A1|2021-01-21|Device for observing a living cell or a set of living cells
    EP2981807B1|2017-04-12|Optical method for characterising a diffractive surface and apparatus for implementing such a method
    FR3054320A1|2018-01-26|DEVICE AND METHOD FOR SAMPLE CHARACTERIZATION BY PWR SPECTROSCOPY IMAGING
    FR3076617A1|2019-07-12|HOLOGRAPHIC IMAGING SYSTEM AND HOLOGRAPHIC IMAGING ANALYSIS METHOD WITH DETECTION OF DEFECTS IN THE OBSERVATION CHAMBER
    FR2995998A1|2014-03-28|Imaging system for reconstruction of optical properties of biological particle e.g. cell, has index adaptation material i.e. oil placed between support and photodetector matrix, where oil is transparent to wavelength of illumination
    同族专利:
    公开号 | 公开日
    WO2016078946A1|2016-05-26|
    FR3028951B1|2017-01-06|
    EP3221688B1|2019-02-20|
    US20170317125A1|2017-11-02|
    US10418399B2|2019-09-17|
    EP3221688A1|2017-09-27|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    US20070263914A1|2006-03-09|2007-11-15|Tessarae Inc.|Microarray imaging system and associated methodology|
    WO2014068003A1|2012-10-30|2014-05-08|Commissariat à l'énergie atomique et aux énergies alternatives|Device for acquiring an image of a sample, comprising a facility for regulating the heating of a support for receiving the sample, and associated imaging system|
    GB0701201D0|2007-01-22|2007-02-28|Cancer Rec Tech Ltd|Cell mapping and tracking|
    US8842901B2|2010-12-14|2014-09-23|The Regents Of The University Of California|Compact automated semen analysis platform using lens-free on-chip microscopy|FR3020682B1|2014-04-30|2016-05-27|Commissariat Energie Atomique|METHOD AND SYSTEM FOR DETECTING AT LEAST ONE PARTICLE IN A BODILY LIQUID, AND ASSOCIATED METHOD FOR DIAGNOSING MENINGITIS|
    FR3082944A1|2018-06-20|2019-12-27|Commissariat A L'energie Atomique Et Aux Energies Alternatives|METHOD FOR OBSERVING A SAMPLE WITH LENS-FREE IMAGING, TAKING INTO ACCOUNT A SPATIAL DISPERSION IN THE SAMPLE|
    FR3082943A1|2018-06-20|2019-12-27|Commissariat A L'energie Atomique Et Aux Energies Alternatives|METHOD FOR COUNTING SMALL PARTICLES IN A SAMPLE|
    FR3086758B1|2018-09-28|2020-10-02|Commissariat Energie Atomique|METHOD AND DEVICE FOR OBSERVING A SAMPLE UNDER AMBIENT LIGHT|
    FR3090107B1|2018-12-18|2020-12-25|Commissariat Energie Atomique|Method of characterizing a particle from a hologram.|
    FR3094988A1|2019-04-12|2020-10-16|Commissariat à l'Energie Atomique et aux Energies Alternatives|Method of early observation of colonies of microorganisms|
    法律状态:
    2015-11-17| PLFP| Fee payment|Year of fee payment: 2 |
    2016-05-27| PLSC| Search report ready|Effective date: 20160527 |
    2016-11-09| PLFP| Fee payment|Year of fee payment: 3 |
    2017-10-30| PLFP| Fee payment|Year of fee payment: 4 |
    2018-10-25| PLFP| Fee payment|Year of fee payment: 5 |
    2019-10-23| PLFP| Fee payment|Year of fee payment: 6 |
    2021-08-06| ST| Notification of lapse|Effective date: 20210705 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1461316A|FR3028951B1|2014-11-21|2014-11-21|LENS-FREE IMAGING SYSTEM COMPRISING DIODE, DIAPHRAGM AND DIFFUSER BETWEEN DIODE AND DIAPHRAGM|FR1461316A| FR3028951B1|2014-11-21|2014-11-21|LENS-FREE IMAGING SYSTEM COMPRISING DIODE, DIAPHRAGM AND DIFFUSER BETWEEN DIODE AND DIAPHRAGM|
    US15/528,055| US10418399B2|2014-11-21|2015-11-09|Lens-free imaging system comprising a diode, a diaphragm, and a diffuser between the diode and the diaphragm|
    EP15791600.8A| EP3221688B1|2014-11-21|2015-11-09|Lens-free imaging system comprising a diode, a diaphragm and a diffuser between the diode and the diaphragm|
    PCT/EP2015/076016| WO2016078946A1|2014-11-21|2015-11-09|Lens-free imaging system comprising a diode, a diaphragm and a diffuser between the diode and the diaphragm|
    [返回顶部]