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    • 专利摘要:
    This method of detecting at least one particle in a body fluid is performed via a detection system comprising a light source, a transparent substrate and a matrix photodetector, the substrate being disposed between the light source and the photodetector. This method comprises placing a drop of body fluid on the substrate, illuminating (100) the drop via the light source, acquiring (110) several successive images of the drop via the photodetector, each image being formed by a radiation transmitted by the illuminated drop and comprising at least one elementary diffraction pattern, each elementary diffraction pattern corresponding to waves diffracted by a particle during the illumination of the drop, the identification (120), via the acquired images, mobile elementary diffraction patterns, and the enumeration (130) of particles moving in the drop, via the identified mobile elementary diffraction patterns.
    公开号:FR3020682A1
    申请号:FR1453959
    申请日:2014-04-30
    公开日:2015-11-06
    发明作者:Cedric Allier；Michel Drancourt
    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] The present invention relates to a method for detecting at least one particle in a body fluid. This detection method is implemented using a detection system comprising a light source, a transparent substrate and a matrix photodetector, the transparent substrate being disposed between the light source and the matrix photodetector. The invention also relates to a method of diagnosing meningitis, comprising determining a number of white blood cells in a predetermined amount of cerebrospinal fluid using such a detection method, the body fluid being the fluid. cerebrospinal fluid and the detected particles being the white blood cells contained in said cerebrospinal fluid. Meningitis is then diagnosed if the number of white blood cells detected in the predetermined amount of cerebrospinal fluid is greater than a predetermined threshold value. The invention also relates to a system for detecting at least one particle in the body fluid. The invention generally relates to the detection of particles, such as cells, in a body fluid, in particular in order to detect an eventual disease as soon as possible. The detection of white blood cells in cerebrospinal fluid allows for example to diagnose cases of meningitis. A known experimental protocol for detecting white blood cells in the cerebrospinal fluid then consists in depositing, on a microscope slide, a drop of approximately 10 μl of the cerebrospinal fluid that was previously taken from the patient, the step sampling is not concerned by the present invention. It is agreed that meningitis is diagnosed if a 10p1 sample of cerebrospinal fluid contains at least 10 white blood cells, these white blood cells being the indirect mark of a viral or bacterial infection. However, counting these white blood cells is a tedious operation for the technician and quite imprecise, since it involves counting the white blood cells using a microscope. A more accurate alternative, but much more expensive, long to implement and requiring bulky equipment, is to use cytometric methods.
    [0002] The object of the invention is therefore to provide a method and a system for detecting particles in the body fluid which is less expensive and easier to implement. From an experimental point of view, the invention then makes it possible to carry out a continuous enumeration of the detected particles, and to diagnose, if appropriate, a particular disease. For this purpose, the subject of the invention is a method for detecting at least one particle in a body fluid, using a detection system comprising a light source, a transparent substrate and a matrix photodetector, the transparent substrate being disposed between the light source and the matrix photodetector, the method comprising the following steps: placing the body fluid in the form of a drop on the transparent substrate, illuminating the drop with the aid of the light source, - the acquisition of several successive images of the drop using the matrix photodetector, each image being formed by a radiation transmitted by the illuminated drop and comprising at least one elementary diffraction figure, each diffraction pattern elementary state corresponding to waves diffracted by a particle during the illumination of the drop, - the identification, from acquired images, of figures of d elementary mobile fraction, and - the enumeration of moving particles within the drop, from the mobile elementary diffraction figures thus identified. According to other advantageous aspects of the invention, the detection method comprises one or more of the following characteristics, taken separately or in any technically possible combination: the method further comprises a step of heating the drop to promote the displacement; particles within the drop; each acquired image comprises a plurality of pixels and the matrix photodetector is adapted to measure the intensity of each pixel, and the step of identification of the mobile elementary diffraction figures comprises: + the determination, for each pixel of the image , the median value or the average value of the intensity of said pixel for a set of acquired images, + the calculation, for at least one acquired image, of a resultant image by subtraction, for each pixel of the image acquired, of said median value or of said average value, and + the detection, on each resultant image, of at least one diffraction pattern, each diffraction pattern detected on the resulting image corresponding to a moving elementary diffraction pattern; the identification step further comprises following each detected elementary diffraction pattern of a resultant image to the next resulting image, each moving elementary diffraction pattern having, between two successive resultant images, a displacement greater than one predetermined minimum distance; the step of identifying mobile elementary diffraction patterns comprises: + detecting, on each acquired image, at least one elementary diffraction pattern corresponding to a particle within the drop, and + following each figure detected elemental diffraction of an acquired image to the next acquired image, each moving elementary diffraction pattern having, between two successive acquired images, a displacement greater than a predetermined minimum distance; the method further comprises a step of characterizing the detected elementary diffraction movement figures and a step of classifying the figures characterized according to at least two distinct categories; the characterization step comprises calculating, for each identified mobile elementary diffraction figure, a ratio between the maximum intensity and the median intensity of a region of interest of the image comprising said elementary diffraction pattern identified mobile, the classification of said diffraction pattern then being performed according to the value of the calculated ratio; the detection step comprises the location in the image of the center of each elementary diffraction figure; the localization in the image of the center of each elementary diffraction figure is carried out via an autocorrelation with a reference elementary diffraction figure; the location in the image of the center of each elementary diffraction figure is made from: + of a reconstruction of an image of the particle associated with said elementary diffraction figure, by implementing a reconstruction algorithm, then + the detection, in the reconstructed image, of the position corresponding to the center of said elementary diffraction figure.
    [0003] The subject of the invention is also a method for diagnosing meningitis comprising the following steps: determining a number of white blood cells in a predetermined quantity of cerebrospinal fluid using a detection method such as defined above, the body fluid being the cerebrospinal fluid and the detected particles being the white blood cells contained in said cerebrospinal fluid, and - the diagnosis of meningitis if the number of white blood cells in the predetermined amount of cerebrospinal fluid -spinal is greater than a predetermined threshold value. The invention also relates to a system for detecting at least one particle in a body fluid, the system comprising: a transparent substrate adapted to receive body fluid in the form of a drop, a light source adapted to emitting a light beam of illumination of the drop, a matrix photodetector adapted to acquire several successive images of the drop, each image being formed by a radiation transmitted by the lighted drop and comprising at least one elementary diffraction figure, each FIG. elementary diffraction corresponding to waves diffracted by a particle during the illumination of the drop, and - an information processing unit adapted to: + identify, from the images acquired, mobile elementary diffraction patterns, + count particles moving within the drop, from the mobile elementary diffraction patterns identified s.
    [0004] The features and advantages of the invention will appear on reading the following description, given solely by way of nonlimiting example, and with reference to the appended drawings, in which: FIG. 1 is a perspective view of FIG. 2 is a schematic representation of the detection system of FIG. 1, the detection system comprising a light source, a transparent substrate adapted to receive the body fluid in the form of a a drop, a matrix photodetector adapted to acquire successive images of the drop and an information processing unit, the information processing unit being configured to identify, from the acquired images, moving elementary diffraction patterns, then to count moving particles within the drop, from the identified mobile elementary diffraction patterns, - FIG. 3 is a flowchart of a detection method according to the invention, FIG. 4 is a view of an image acquired with the aid of the photodetector of FIG. 2, during the illumination of a drop of liquid. Figure 5 is a view of a resultant image obtained from the acquired image of Figure 4 and subtracting, at the value of the intensity of each pixel of the acquired image, from a median value of the intensity of said pixel, the median value being determined for a set of acquired images, - Figure 6 is an enlargement of the boxed area VI of Figure 5, - Figure 7 is an image illustrating a follow-up diffraction patterns, the white dots corresponding to the successive positions of the centers of said diffraction patterns; FIG. 8 is a set of dots representing the number of white blood cells detected in the cerebrospinal fluid drop, with the abscissa being the number of white blood cells determined to using a method of cytometry and ordinate that determined using the system and detection method according to the invention, each point corresponding to a sample of cerebrospinal fluid of a respective patient, - Figure 9 is a set of views obtained using the photodetector of FIG. 2 for the same sample of cerebrospinal fluid, each containing a diffraction pattern corresponding to a respective white blood cell; FIG. 10 is a set of points representing each a ratio between the maximum intensity and the median intensity of a region of interest of a respective view of FIG. 9 having a corresponding diffraction pattern; FIG. 11 is a view similar to that of FIG. 10, with several cerebrospinal fluid samples from different patients, and - Figure 12 is a set of two curves, one for a white blood cell and the other for a red blood cell, each curve represents nt an intensity profile near the center of the diffraction pattern as a function of a distance expressed in i..tm, the center of the diffraction pattern corresponding to the distance equal to 225 iim.
    [0005] In the remainder of the description, the expression "substantially equal to" defines a relation of equality to plus or minus 5 ° Vo. In FIGS. 1 and 2, a particle detection system 22 contained in a body fluid 24 comprises a transparent substrate 26 adapted to receive the body fluid 24 in the form of a drop 28. The detection system 20 also comprises a light source 30 and a matrix photodetector 32 adapted to acquire several successive images of radiation transmitted by the drop 28 illuminated by the light source 30. The detection system 20 is generally adapted to detect the particles 22 in the liquid body 24 via a methodology without lens imaging, the matrix photodetector 32 having no magnification optics. The detection 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. In addition, the detection system 20 optionally comprises a device 40 hinged doors, the doors being painted black, to isolate the radiation transmitted by the illuminated drop 28 of 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 detection system.
    [0006] The detection 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 diffractive particles 22 are, for example, biological particles, that is to say cells (especially blood cells and for example white blood cells or red blood cells), bacteria or bacterial columns, or aggregates of cells. The diffracting particles 22 generally have a diameter of less than 100 μm. The diameter of the diffracting particles 22 is, for example, between 1 μm and 100 μm. The cells, such as white blood cells and red blood cells, have a diameter of the order of 10 .mu.m. The body fluid 24 is a liquid that has previously been removed from a patient, the sampling step not being part of the perimeter of the invention. The body fluid 24 is for example cerebrospinal fluid when the detection system 20 is intended to diagnose meningitis.
    [0007] The transparent substrate 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 direction of illumination of the body fluid 24 by the light source 30, as shown in FIG. 2. The transparent substrate 26 comprises, for example, a transparent blade 48.
    [0008] In this example, the transparent substrate 26 is deposited at the bottom of a petri dish 46. The transparent blade 48, made of a material such as glass, serves to control a wetting angle of the drop 28 so that it does not not stretch too much, to facilitate its observation by imagery without lens in its entirety. The wetting angle, also called the contact angle, corresponds to the angle between the transparent plate 48 and the concave surface of the droplet 28 at the outer periphery of the drop. Preferably, the wetting angle of the drop is less than 90 °, and more preferably substantially between 30 ° and 60 °. The Petri dish 46 here has a function of confining the body fluid 24, in order to protect the external medium with respect to the liquid. It 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 body fluid 24.
    [0009] The drop 28 has for example a volume substantially equal to 10 .mu.L, such a volume being generally used for a cerebrospinal fluid sample in the case of the diagnosis of meningitis. The light source 30 is adapted to emit a light beam 50 in the vertical direction Z in order to illuminate the body fluid 24 comprising the diffracting particles 22. The light source 30 is disposed at a first distance D1 from the transparent plate 48 according to the vertical direction Z. The first distance D1 preferably has a value of between 1 cm and 30 cm, for example equal to 5 cm. 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 comprises, for example, a point source such as a light emitting diode 52, also called LED (Light Emetting Diode), and a diaphragm 54 disposed in contact with the LED 52, as shown in FIG. schematic in Figure 2. The diaphragm 54 has a diameter of between 50 lm and 500 iim, preferably substantially equal to 150 iim. This makes it possible to increase the spatial coherence of the light radiation. The LED 52 has for example a wavelength substantially equal to 617 nm. Alternatively, the light source 30 consists of the light emitting diode 52, and has no diaphragm. The electroluminescent diode 52 then has sufficiently small dimensions to be considered as spatially coherent, the diameter of the light emitting diode 52 then being for example less than one-tenth of the first distance D1. In another variant, the light source 30 is a spatially and temporally coherent light source, for example a laser diode or a VCSEL (Vertical Cavity Surface Emitting Laser) type laser diode.
    [0010] The matrix photodetector 32 is adapted to acquire successive images of the radiation transmitted by the body fluid 24 in the form of a drop 28 containing the diffracting particles 22, illuminated by the light beam 50. By transmitted radiation is meant radiation passing through the body fluid 24 such that the matrix photodetector 32 and the light source 30 are located on either side of the body fluid 24 comprising the diffracting particles 22. 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 28 is a CCD (Charge Coupled Device) sensor. The matrix photodetector 32 comprises a plurality of pixels, not shown, each having dimensions less than or equal to 10 i..tm. In the embodiment of FIGS. 1 and 2, each pixel is in the form of a square with a side substantially equal to 2.2 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 transparent substrate 26 and the photodetector 32. The images acquired by the matrix photodetector 32 are formed by the transmitted radiation. directly by the illuminated body fluid 24, in the absence of magnification optics disposed between the transparent substrate 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 vertical direction Z, and the second distance D2 is then less than a few centimeters, preferably less than 1 cm, and for example equal to 700 μm. 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 transparent substrate 26, makes it possible to limit the phenomena of interference between different diffraction figures when the liquid body 24 is illuminated.
    [0011] The matrix photodetector 32 is then able to make an image of at least one elementary diffraction pattern 60 transmitted by the body fluid 24, each elementary diffraction pattern 60 corresponding to waves diffracted by a diffractive particle 22, during the illumination of the body fluid 24 in the form of the drop 28. Thus, the matrix photodetector 32 makes it possible to obtain an image ln, called the observed image, comprising one or more elementary diffraction figures 60, where n is an index comprised between 1 and N and corresponding at the number of the image in the sequence of successive images acquired, with n and N integers greater than or equal to 1. The acquisition rate is generally between 50 images per second and one image every 10 to 20 seconds. FIG. 4 represents a plurality of elementary diffraction patterns 60 corresponding to white globules, each figure consisting of a central zone whose intensity is substantially homogeneous, this central zone being surrounded by concentric rings whose intensity is alternatively weak (dark rings) and high (light rings). Each image acquired In by the matrix photodetector 32 comprises a plurality of pixels In (x, y), each being marked by an abscissa x and an ordinate y in the image 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 detecting particles 22 in the body fluid 24. The processor 38 is adapted to execute the detection software 70. The detection software 70 forms a means for detecting particles 22 in the liquid 24. In a variant, the detection means 70 are made in the form of programmable logic components or in the form of dedicated integrated circuits. The detection software 70 is adapted to identify, from the acquired images 11, 1'1, moving elementary diffraction patterns 60, and to count moving particles 22 within the drop 28, from the elementary diffraction patterns identified mobile. In order to identify the mobile elementary diffraction patterns, the detection software 70 is for example adapted to detect, on each acquired image In, at least one elementary diffraction pattern 60 corresponding to a particle 22 within the drop 28, then adapted to follow the position of each detected elemental diffraction pattern 60 of an acquired image In at a time tn, to an image 1 ', acquired at a time t', i being an integer index generally between 1 and 10. Preferably, the index i is equal to 1 and the evolution of the position of each detected elementary figure 60 between two consecutive images ln and In + 1 is then detected.
    [0012] By position tracking is meant the tracking of the position of a point of the elementary diffraction pattern 60 between two images ln and In + ,. This point may for example be a center 74 of the elementary diffraction pattern 60. In general, a diffraction pattern is considered to be in motion if between two acquired images ln, ln +, the diffraction pattern moves according to a distance greater than a predetermined minimum distance Dmin.
    [0013] The predetermined minimum distance Dmin is, for example, greater than 5 pixels, or even 10 pixels, for a time difference of the order of one second, between the acquisition instants tn, tn ± i. Thus, the detection software 70 makes it possible to detect moving elementary diffraction patterns 60, each of which corresponds to a particle moving in the liquid. In order to identify the mobile elementary diffraction patterns, the detection software 70 is alternatively adapted to determine, for each pixel, an image, called the lbackground background image, corresponding to a stationary component of a set of images 1 at p, where m is a particular value of the index n, p is an integer greater than 1, generally between 3 and 10, and for example equal to 5. The detection software 70 is then adapted to computing, for each image acquired ln, a resultant image n by subtraction for each pixel In (x, y) of the acquired image of the value of the pixel lbackground (x, y) of the background image 'determined background . Thus, the n (x, y) = In (x, y) - 'background (X5Y) (1) The resulting image n then shows the moving component of each of the images ln including the elementary diffraction patterns 60, and the detection software 70 is adapted to detect, on each resulting image n, one or more diffraction patterns, each diffraction pattern detected on the resulting image n corresponding to a moving elementary diffraction pattern.
    [0014] The background image is, for example, an image, called the median image 1'd, where each pixel 1'd (x, y) has the value of the median value of the pixels I, (x, y),. 1'p (x, y) of the set of images 1, to 1'p. In other words, background (x, Y) = Imed (X, y) = me d [Ini (x, y) ... Im + p (x, y)] (2) where med denotes the median operator.
    [0015] The images p 1 at 1'p can precede the image In. Alternatively, the image In can be part of the set of p images whose background image is calculated. The background image then represents a reference image, on which the movements of the elementary diffraction patterns, visible on the images 1, 1'p are erased or attenuated. Thus, the background image background can be considered as the image of a background common to each of the images 1, 1'p, corresponding to the immobile component of each of these images.
    [0016] Alternatively, the background image I b'kgro'd is obtained by calculating the average value of each pixel of the set of images 1, to 1p. In other words: background (x, Y) = Imean (x, Y) = me an [lm (x, y) ... m + p (x, y)] (3) where mean is the mean operator, m is a particular value of the index n, p is an integer greater than 1, generally between 3 and 10, and for example equal to 5. In addition, the resulting image 1c thus calculated is used to follow the position of each detected elementary diffraction pattern 60. In other words, according to this optional complement, the detection software 70 is for example adapted to detect the diffraction patterns , follow the position of the diffraction patterns and count the moving particles 22 in the drop 28 according to the moving elementary diffraction patterns, from the resultant images 1 ', instead of the acquired images 1 ,, with the index n varying between 1 and N. Thus, it is possible to identify the elementary diffraction patterns 60 moving between two images 1 ,, 1 ',. Their enumeration makes it possible to estimate the number of moving particles in the liquid 24. An important aspect of the invention is therefore the discrimination between the immobile elementary figures and the mobile elementary diffraction figures, the latter being counted to estimate the number of particles. particles in the liquid.
    [0017] When the liquid 24 to be analyzed is in the form of a drop 28, the convection currents allow the particles 22 to move in the drop. The detection of these particles, and their enumeration, makes it possible to avoid the detection of parasitic elements not present in the drop 28, but which can generate elementary diffraction patterns on the photodetector and, consequently, distort the measurement. Such elements are, for example, dust or even scratches, present on the transparent support 26, on the confinement element 46 or on the surface of the photodetector 32. By counting only the particles 22 in motion, it is avoided to take into account of these immobile elements, which generate fixed, that is to say motionless, diffraction patterns, unlike particles moving in the drop.
    [0018] It should be noted that the increase in temperature of the drop 28 makes it possible to amplify the convection currents within the drop 28, which increases the mobility of the particles 22 present in the latter. Because of the proximity between the drop 28 and the photodetector 32, the temperature of the drop 28 tends to increase towards a temperature between 40 ° Celsius and 50 ° Celsius, thereby promoting the movement of the particles 22.
    [0019] Also, in general, it is preferable that the liquid to be analyzed 24 is mobile, and in particular deposited in the form of the drop 28, deposited on the transparent substrate 26 and exposed to the open air: this allows a movement spontaneous particles 22 in the drop 28. The provision of body fluid 24 in the form of the drop 28 has many advantages: - a volume of the order of a few pl to a few tens of pl, high enough to establish a reliable diagnosis, - spontaneous movement of the particles 22 to be detected, - simplicity of implementation, a simple deposit being sufficient, - compatibility with an observation without lens imaging, depth of field of up to several centimeters: all the particles 22 present in the drop produce an exploitable diffraction pattern 60. In addition optional, the detection software 70 is adapted to characterize the mobile elementary diffraction patterns identified. The term "characterize" refers to the determination of a quantitative parameter relating to an elementary diffraction pattern. An example of such a parameter will be described later. In optional addition, the detection software 70 is also adapted to sort the detected elementary diffraction patterns 60 according to at least two distinct categories, in order to classify the particles 22 corresponding to the detected elementary diffraction patterns 60 according to at least two distinct classes, each class being associated with a respective category. The sorting, also called classification, is performed according to a parameter determined during the characterization phase of the particles. In particular, in order to follow the position of the diffraction patterns, the detection software 70 is adapted to locate, in the acquired image In or in the resulting image n, a particular point, for example the center 74, of each FIG. elemental diffraction 60, as shown in FIGS. 4 and 6. The location of each particular point, such as the center 74, is for example performed by applying an autocorrelation function, preferably standardized, so as to obtain, from of the observed image ln and of a reference diffraction pattern IR, of a correlation image lc, satisfying the following equation: / R (i, j) x (x + i, y + j) Ic (x, Y) = (4). ## EQU1 ## On the correlation image 1c, each peak of intensity then corresponding to the position of the center 74 of the diffraction pattern corresponding to the reference image IR.
    [0020] The elementary reference diffraction pattern IR is previously established, on the basis of modeling or on the basis of experimental images. Alternatively, to detect the center 74 of the diffraction pattern, the detection software 70 is adapted to reconstruct an image of the diffracting particles 22 from the acquired image 1n or the resulting image n, and following a known holographic reconstruction algorithm. Such an algorithm makes it possible, from an elementary diffraction pattern, to reconstruct the geometry and / or the position of the diffracting object. The detection software 70 is then able to detect in the reconstructed image the position corresponding to the center 74 of each diffraction pattern, then to determine a region of the acquired image 1n or resultant n, this region comprising the FIG. corresponding elementary diffraction 60. The detection software 70 is finally able to detect the center 74 of the diffraction pattern by correspondence with the position detected in the reconstructed image. The implementation of such an algorithm requires however a control of the geometry of the liquid. It applies especially when analyzing a liquid filling a fluidic chamber, the liquid being set in motion in said chamber. As a variant, the center 74 of an elementary diffraction pattern 60 is determined manually, the operator making a manual selection of the zone of the image considered as representative of the central zone of a corresponding elementary diffraction pattern 60 From the coordinates, in the image I n, of the center 74 of each elementary diffraction pattern thus identified, for example, a region of interest 76 is defined around this center 74, as shown in FIGS. region of interest 76 typically comprises from 10 to 1000 pixels, preferably from 10 to 100 pixels.
    [0021] The detection software 70 is adapted to track the position of each detected elemental diffraction pattern 60 from an acquired image 1n to the next acquired image 1'1, or respectively from a resultant image n resulting image following the n + 15 using a cell tracking method which consists for example in pairing in two successive images ln, In + 1, n, l 'n + 1, the nearest particles. Such a cell tracking method is for example described in the article "Automated tracking of migrating cells in phase-contrast video microscopy sequences using image registration" of Hand A. J .; Sun T .; Barber D. C .; Hose D. R, MacNeil S., published in the journal Journal of Microscopy in 2009, Vol. 234, pp. 62-79.
    [0022] The detection software 70 is then adapted to determine, among the elementary diffraction patterns followed 60, the mobile diffraction patterns, the displacement between two successive acquired images ln, In + 1, respectively between two successive successive images. n + 1, is greater than the predetermined minimum distance Dmin, the particles corresponding to these mobile elementary diffraction patterns 60 then being considered as particles in movement within the drop 28. The detection software 70 is furthermore adapted to counting the particles in movement within the drop 28, that is to say the one whose displacement of the corresponding diffraction figures is greater than the predetermined minimum distance Dmin- The detection software 70 is, in addition optional, adapted for characterize each identified elementary mobile diffraction pattern 60, that is, determine one or more criteria es 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 the region of interest 76 of said diffraction pattern. Examples of value of the ratio R for different diffraction patterns 60, each associated with a corresponding region of interest 76, are illustrated in FIGS. 10 and 11.
    [0023] The detection 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 then performed by comparing the calculated ratio R with at least one predetermined threshold. In other words, according to this exemplary embodiment, a classification criterion of the figures is a comparison relation of the calculated ratio R with one or more corresponding predetermined thresholds. The operation of the detection system 20 according to the invention will now be described with reference to FIG. 3 representing a flowchart of the detection method according to the invention. During the initial step 100, the body fluid 24 is deposited in the form of the drop 28 on the transparent substrate 26, in particular on the transparent slide 48. In the embodiment described, and in order to diagnose meningitis, the body fluid 24 is cerebrospinal fluid, and the amount of body fluid deposited on the transparent substrate 26, in the form of a drop 28, is for example equal to 10 .mu.m. The transparent blade 48 is itself placed at the bottom of the petri dish 46 in order to control the spreading of the drop 28 on the blade 48. The drop 28 of body fluid is then illuminated with the help of the light source. 30 spatially coherent, the light beam 50 being directed in the vertical direction Z.
    [0024] In step 110, the matrix photodetector 32 performs the sequential acquisition of several transmission images ln, ln +, at successive instants tn, f .n, - + 1- Each transmission image ln, ln + is formed by the radiation transmitted, at the time of acquisition t .n, f -n + 1, corresponding, by the body fluid 24 illuminated. In other words, the matrix photodetector 32 makes images of the elementary diffraction patterns 60 transmitted by the particles in the illuminated body fluid 24, each elementary diffraction pattern corresponding to waves diffracted by the diffracting particles 22 during illumination of the liquid 24, these diffracted waves interfering with the incident light wave.
    [0025] The number of acquired images ln is for example equal to 10, and the number N is then equal to 10. The observation of an exploitable diffraction figure, by placing the matrix photodetector 32 at a relatively small distance is notably due to the absence of magnification optics between the body fluid 24 and the matrix photodetector 32.
    [0026] During the acquisition step 110, the photodetector 32 is preferably arranged at a small distance from the body fluid 24, the second distance D2 between the body fluid 24 and the photodetector 32 in the vertical direction Z being, for example, order of a few millimeters, and preferably less than 1 cm. At the end of the acquisition step 110, the detection software 70 performs, during the step 120, the identification, from the acquired images ln, In + 1, of mobile elementary diffraction patterns 60. This step 120 of identification of mobile diffraction patterns will be described in more detail later. In the next step 130, the detection software 70 realizes the enumeration of the moving particles 22 within the drop 28, from the mobile elementary diffraction figures thus identified. In optional complement, the detection software 70 can implement, during the step 140, the characterization of the detected elementary diffraction patterns corresponding to the moving particles according to at least two distinct categories, in order to classify, during the step 150, the moving particles associated with these detected elementary diffraction patterns. The characterization step 140 will be described in more detail later. To identify mobile diffraction patterns in step 120, three methods will now be described. According to a first method, represented in FIG. 3 by the continuous line routing inside step 120, the detection software 70 determines, during a substep 200, for each pixel (x, y), a median value, or alternatively a mean value, of the intensity of said pixel for a set of acquired images 1, at 1'p, and preferably for all the acquired images, i.e. images ln with n between 1 and N. We then establish the background image 'background previously defined according to equation (2), or alternatively according to equation (3).
    [0027] The detection software 70 then calculates, again during this substep 200, for each acquired image of said set, preferably for each of the images acquired, the resulting image n by subtraction according to the equations (1) and (2 ), to the measured value of the intensity of each pixel of the acquired image ln, of the median value previously determined, or alternatively of the average value according to equations (1) and (3) above. The calculation of these resulting images n by subtraction of the median value, or alternatively of the average value, of each of the pixels makes it possible to visualize the mobile elementary diffraction figures, the so-called immobile component of the In image being removed. , or, at least, attenuated. These mobile diffraction patterns correspond to the particles 22 moving in the drop 28. In other words, the resulting images n allow to identify the moving particles in the drop 28. This is also clearly visible by comparing Figure 4 corresponding to an image acquired ln, with FIGS. 5 and 6 corresponding to the resulting image n associated with the acquired image of FIG. 4. In FIG. 5, only the moving particles of FIG. 4 appear. Moreover, it can be seen that the only diffraction figures visible in FIG. 5 are situated inside an area corresponding to the drop 28 (the outer periphery of the drop 28 being in the shape of a fairly wide peripheral rim on FIGS. 4 and 5), whereas in FIG. 4 corresponding to the acquired image, diffraction patterns are visible both inside the zone corresponding to the drop 28 and outside this zone corresponding to the drop 28. After the sub-step 200, the detection software 70 detects, during the sub-step 210, on each resulting image the n, each elementary diffraction pattern 60 corresponding to a particle 22 within the droplet 28. For this purpose, the detection software 70 performs, for example, as described above, a comparison between the resulting image and a reference diffraction pattern by an autocorrelation, preferably standardized, between said image and the reference diffraction pattern, each intensity peak in the obtained autocorrelation image corresponding to the center position 74 of a corresponding diffraction pattern. Alternatively, as previously described, the location in the image of the center 74 of each elementary diffraction pattern 60 is made from a reconstruction of an image of the particle 22 associated with the corresponding elementary diffraction pattern 60 by implementing a known algorithm of reconstruction, then of the detection, in the reconstructed image, of the position corresponding to the center of said elementary diffraction pattern 60. In another variant, the detection of the center 74 of each elementary diffraction pattern 60 is performed manually by the operator, the latter performing a manual selection of the area of the image considered representative of the central zone of the diffraction pattern. In another variant, the center 74 of each elementary diffraction pattern 60 is obtained by thresholding operations of the gray levels, and then Boolean operations applied to the thresholded image. Once the diffraction patterns are detected, each corresponding to a particle 22 moving in the drop 28, the detection software 70 then counts the moving particles within the drop 28 of body fluid, during the step 130 that follows sub-step 210 according to the first method of identification of mobile diffraction patterns. According to a second identification method, represented in FIG. 3 by the dotted line path inside step 120, the detection software 70 always calculates, during the sub-step 200, the resulting image 1, of each acquired image 1 ,, and then detects in the sub-step 210 the diffraction patterns in the resulting image n.
    [0028] According to the second method, the detection software 70 additionally performs, during a substep 220, the tracking of a resultant image 1 'to the next resulting image G + of each detected diffraction pattern. This sub-step is performed by applying a cell tracking algorithm, as described above, such as the algorithm described in the aforementioned article by Hand et al.
    [0029] This second method then allows an even more reliable identification of the mobile diffraction patterns corresponding to the particles in motion in the drop 28. During the step 130 which follows the substep 220 according to this second identification method, the detection software 70 then counts the moving particles within the body fluid drop 28, that is to say the particles 22 whose corresponding elementary diffraction patterns 60 have made a displacement greater than the predetermined minimum distance Dmin between two successive acquisitions corresponding to instants -n, tn + 1. The displacement of each elementary diffraction pattern 60 of a resulting image 1 'to the other G + is preferably calculated by measuring the displacement of the center 74 of said figure of an image 1' to the other. n + 1.
    [0030] Counting the moving particles within the drop 28 by further tracking the diffraction patterns from the resulting images, n, 1 ', allows the number of moving particles to be determined more accurately. in the drop 28.
    [0031] According to a third identification method, represented in FIG. 3 by the mixed-line routing inside step 120, the calculation of the resulting image is not carried out, and the process goes directly from the step 110 to sub-step 210 in which the detection software 70 detects, on each acquired image ln with n varying between 1 and N, each elementary diffraction pattern 60 corresponding to a particle 22 within the drop 28. This detection is carried out in the same manner as previously described for the detection of the diffraction patterns in each resulting image n, with the difference that, according to this third identification method, the detection is here carried out in each acquired image. According to this third identification method, the detection software 70 then performs, during the following substep 220, the tracking of an acquired image ln, with the following acquired image In +1, of each diffraction pattern detected. This sub-step is performed by applying the cell tracking algorithm, as previously described, such as the algorithm described in the aforementioned article by Hand et al. The tracking of the diffraction patterns 60 in the acquired images ln is illustrated in FIG. 7, where the white dots correspond to the successive positions of the centers 74 of said diffraction figures. In the step 130 following the sub-step 220 according to this third method of identification, the detection software 70 then counts the moving particles within the body liquid droplet 28, that is to say the particles 22 whose corresponding elementary diffraction patterns 60 have moved more than the predetermined minimum distance Dmin between two successive acquisitions corresponding to the instants t-n, -n + 1. This third identification method then makes it possible to identify the mobile diffraction patterns directly in the images acquired, without having to calculate the background image, while obtaining sufficiently reliable results to enable the early detection of a possible disease, for example to diagnose cases of meningitis. The method of detecting particles according to the invention, and enumeration of moving particles within the drop 28, makes it possible to determine, for example, the number of white blood cells in a predetermined quantity of cerebrospinal fluid, the liquid body 24 being the cerebrospinal fluid and the detected particles 22 being the white blood cells contained in said cerebrospinal fluid.
    [0032] Determining the number of white blood cells in a predetermined amount of cerebrospinal fluid then makes it possible to diagnose meningitis, since it is generally considered that meningitis is diagnosed if the number of white blood cells present in a predetermined amount cerebrospinal fluid is greater than a predetermined threshold value. The predetermined threshold value is for example equal to 10 when the predetermined quantity of cerebrospinal fluid is substantially equal to 10 μl. In addition, during step 110 of acquiring successive images of the illuminated drop 28, the drop 28 is further heated to promote the movement of the particles 22 within the drop 28. The heating of the drop 28 is for example implemented using the matrix photodetector 32, the latter forming a heat source. In the embodiment of Figure 1, the heating of the drop 28 is for example obtained by reducing the cooling carried by the heat sink 42 and the fan 44, to cause a slight heating of the photodetector matrix 32, then the drop 28 located near said photodetector 32. The heating of the drop 28 is for example of the order of a few degrees Celsius relative to the ambient temperature, the temperature of the drop 28 being for example between 40 ° Celsius and 50 ° Celsius. FIG. 8 then shows that the results obtained using the detection method according to the invention are consistent with the results obtained via a reference method for particle counting, in this case cytometry. The detection method according to the invention makes it possible to effectively identify body fluid samples 24 having a large number of moving particles relative to body fluid samples 24 having few moving particles 22.
    [0033] In the example of Figure 8, the body fluid 24 is cerebrospinal fluid and the detected moving particles 22 are white blood cells. For each cerebrospinal fluid sample represented by a rhombus, the number on the abscissa corresponds to the number of white blood cells determined by the reference method by cytometry and the number on the ordinate corresponds to the number of white blood cells determined using the method of detection according to the invention. For a first sample of cerebrospinal fluid corresponding to the rightmost rhombus in FIG. 8 (sample 1 of the table below), the determined number of white blood cells via the detection method according to the invention is equal to 89 and the number of white blood cells determined for the same sample with a cytometry method is equal to 44. For a second sample corresponding to the diamond located in the middle of Figure 8 (sample 7 of the table below), the number of white blood cells determined with the detection method according to the invention is equal to 37, and that determined by cytometry for this same sample is equal to 12. For the other samples of cerebrospinal fluid (samples 2 to 6 of the table below), corresponding to the diamonds on the left of FIG. 8, the determined number of white blood cells is small, for example less than or equal to 10, whether with the method according to invention or by cytometry, and corresponds to an absence of meningitis. The results of the number of white blood cells determined using the detection method according to the invention and according to the cytometry method are furthermore indicated in the table below for each sample of body fluid tested.
    [0034] Sample number Number of white blood cells Number of white blood cells by cytometry according to the invention 1 44 89 2 1 2 3 0 2 4 2 6 5 0 20 6 1 11 7 12 37 Table 1 Even if the number of particles in motion detected with the process according to the invention is relatively different from the number of particles detected by cytometry in the body fluid drop 28, the detection method according to the invention nevertheless makes it possible to discriminate a body fluid 24 comprising a large number of particles in motion by compared to a body fluid 24 with few moving particles, so that a diagnosis associated with the body fluid 24 taken, such as the diagnosis of meningitis, remains satisfactory as shown in Figure 8. Of course, this method is still refining but we can already say that when the number of particles exceeds a certain threshold, such as a threshold of 20 white blood cells in a volume of 1..1L, a complementary analysis by a reference method is recommended. Thus, this method, simple to implement, fast and inexpensive, is an aid to effective diagnosis.
    [0035] The characterization step 140 is for example performed using the calculation of the ratio R between the maximum intensity and the median intensity of the region of interest 76 of the image comprising said diffraction pattern. Such a characterization is illustrated in Figures 10 and 11 for which the body fluid 24 is cerebrospinal fluid, and the particles to be classified are globules, to be classified according to two distinct classes, namely white blood cells and red blood cells.
    [0036] In FIG. 11, column A corresponds to white blood cells, and the values of the ratio R, associated with column A in the ordinate and calculated for the different diffraction figures corresponding to the white blood cells, are between approximately 1.5 and 2. 8. More precisely, the R ratio values are most frequently greater than 1.75 when the diffraction patterns correspond to white blood cells. This is confirmed by FIGS. 9 and 10, with FIG. 9 showing the diffraction patterns obtained on the sample of a patient with meningitis, which sample contains only white blood cells according to a cytometry measurement performed in parallel. FIG. 10 illustrates the R-ratio values calculated for each of the diffraction patterns, the R-ratio values ranging from 1.5 to 2.8, mainly from 1.75 to 2.8.
    [0037] In FIG. 11, column B corresponds to red blood cells, and the values of the ratio R, associated with column B in the ordinate, are between 1 and 2.25, and generally less than 1.75. In other words, with a predetermined threshold equal to 1.75 in the example of FIG. 11, the calculation of the ratio R will make it possible to discriminate red blood cells from white blood cells fairly effectively, white blood cells being considered as moving particles. for which the associated ratio R is greater than the predetermined threshold, chosen equal to 1.75, and the red blood cells being considered as moving particles for which the associated ratio R is less than the predetermined threshold. Thus, the method may comprise a step 150 of classification of the detected particles, according to the established characterization criterion, for each of them, during the characterization phase. This difference in ratio R between the white blood cells and the red blood cells is also visible in FIG. 12, where the curve 200 represents an intensity profile near the center 74 of the diffraction pattern associated with a white blood cell, as a function of a distance expressed in pm, the center 74 of the diffraction pattern corresponding to the distance substantially equal to 225 pm. Curve 210 similarly represents an intensity profile in the vicinity of the center 74 of the diffraction pattern corresponding to a red blood cell, as a function of the distance expressed in μm, the center 74 also corresponding to the distance substantially equal to 225 μm. .
    [0038] It can be seen that the maximum intensity of the diffraction pattern associated with the white blood cell is greater than that associated with the red blood cell, whereas the median intensity of the diffraction pattern is substantially equal for the white blood cell and for the globule. red, so that the ratio R is higher with the white blood cell than with the red blood cell. The classification carried out in step 150 between two types of particles, such as for example between white blood cells and red blood cells, then makes it possible to distinguish the two forms of meningitis, namely infectious meningitis and meningeal hemorrhage. Infectious meningitis corresponds to the case where moving particles are white blood cells, and meningeal haemorrhage corresponds to that in which the particles in motion are red blood cells.
    [0039] It is thus conceivable that the method and the detection system 20 according to the invention make it possible to detect the particles 22 in motion in the body fluid 24 in a particularly inexpensive and easy to implement manner. This then makes it possible to continuously count the particles detected, and to diagnose any particular disease, such as meningitis, if necessary.
    权利要求:
    Claims (12)
    [0001]
    CLAIMS 1. A method for detecting at least one particle (22) in a body fluid (24), using a detection system (20) comprising a light source (30), a transparent substrate (26). ) and a matrix photodetector (32), the transparent substrate (26) being disposed between the light source (30) and the matrix photodetector (32), the method comprising the following steps: - placing the body fluid (24) under form of a drop (28) on the transparent substrate (26), - the illumination (100) of the drop (28) with the aid of the light source (30), - the acquisition (110) of several successive images (1 ,, 1 ',) of the drop (28) using the matrix photodetector (32), each image (1') being formed by a radiation transmitted by the illuminated drop (28) and comprising least one elementary diffraction pattern (60), each elementary diffraction pattern (60) corresponding to waves diffracted by a particle (22) during the illumination of the drop (28), - the identification (120), from the acquired images (I ', In + 1), of mobile elementary diffraction patterns (60), - the enumeration (130) of particles (22) moving within the drop (28), from the mobile elementary diffraction patterns thus identified.
    [0002]
    2. The method of claim 1, wherein the method further comprises a step of heating the drop (28) to promote the movement of particles (22) within the drop (28).
    [0003]
    The method of claim 1 or 2, wherein each acquired image (I,) has a plurality of pixels (I, (x, y)) and the matrix photodetector (32) is adapted to measure the intensity of each pixel (I, (x, y)), and wherein the step (120) for identifying mobile elementary diffraction patterns comprises: - the determination (200), for each pixel (I, (x, y)) of the image (I,), the median value (I'd (x, Y)) or the average value (Imean (x, Y)) of the intensity of said pixel for a set of acquired images ( 1 ,, ..., In + p), - calculating (200), for at least one acquired image (I,), of a resultant image (1 ',) by subtraction, for each pixel (I, x, y)) of the acquired image, said median value (Imed (x, Y)) or said average value (Imean (x, Y)), and the detection (210), on each resulting image ( n), at least one diffraction pattern, each diffraction pattern detected on the resulting image (n) corresponding to a diffractive pattern n elementary mobile.
    [0004]
    The method of claim 3, wherein the identifying step (120) further comprises tracking (220) each detected elemental diffraction pattern of a resulting image (n) to the resulting image. next (1'n + 1), each moving elementary diffraction pattern having, between two successive resultant images (n, a displacement greater than a predetermined minimum distance (Drain) -
    [0005]
    5. A method according to claim 1 or 2, wherein the step (120) for identifying mobile elementary diffraction patterns comprises: detecting (210), on each acquired image (ln), of at least one elementary diffraction pattern (60) corresponding to a particle (22) within the drop (28), and - tracking (220) of each detected elementary diffraction pattern (60) of an acquired image (1n) at the acquired image following (ln-0), each movable elementary diffraction figure having, between two successive acquired images (ln, In + 1), a displacement greater than a predetermined minimum distance (Drain) -
    [0006]
    The method according to any one of the preceding claims, wherein the method further comprises a step (140) of characterizing the detected motion elementary diffraction patterns (60) and a step (150) of classification of the characterized figures according to at least two distinct categories.
    [0007]
    7. The method according to claim 6, wherein the characterization step (140) comprises computing, for each identified mobile elemental diffraction figure, a ratio (R) between the maximum intensity and the median intensity. a region of interest (76) of the image comprising said identified movable elementary diffraction pattern, the classification of said diffraction pattern then being performed as a function of the value of the calculated ratio (R).
    [0008]
    The method of any one of claims 3 to 5, wherein the detecting step (210) includes locating in the image (ln) the center (74) of each elemental diffraction pattern (60). 35
    [0009]
    9. The method of claim 8, wherein the location in the image (I) of the center (74) of each elementary diffraction pattern (60) is performed via autocorrelation with a reference elementary diffraction pattern.
    [0010]
    10. The method of claim 8, wherein the location in the image (ln) of the center (74) of each elementary diffraction figure (60) is made from: - a reconstruction of an image of the particle associated with said elementary diffraction pattern, by implementing a reconstruction algorithm, and then - detecting, in the reconstructed image, the position corresponding to the center of said elementary diffraction pattern.
    [0011]
    11. A method of diagnosing meningitis, comprising the following steps: determining a number of white blood cells in a predetermined quantity of cerebrospinal fluid using a detection method according to any one of preceding claims, the body fluid (24) being the cerebrospinal fluid and the detected particles (22) being the white blood cells contained in said cerebrospinal fluid; - the diagnosis of meningitis if the number of white blood cells detected in the quantity predetermined amount of cerebrospinal fluid is greater than a predetermined threshold value.
    [0012]
    12. A system (20) for detecting at least one particle (22) in a body fluid (24), the system (20) comprising: - a transparent substrate (26) adapted to receive the body fluid (24) under form of a drop (28), - a light source (30) adapted to emit a light beam (50) of illumination of the drop (28), - a matrix photodetector (32) adapted to acquire several successive images ( I ,, l ') of the drop (28), each image (ln) being formed by a radiation transmitted by the illuminated drop (28) and comprising at least one elementary diffraction figure (60), each elementary diffraction figure (60) corresponding to waves diffracted by a particle (22) during the illumination of the drop (28), and - an information processing unit (34) adapted to: + identify, from the images acquired ( ln, l '), mobile elementary diffraction patterns (60), + enumerate particles (22) in motion at within the drop (28), from the identified mobile elementary diffraction patterns.
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    同族专利:
    公开号 | 公开日
    EP3137874A1|2017-03-08|
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    US9970858B2|2018-05-15|
    US20170045439A1|2017-02-16|
    EP3137874B8|2019-06-12|
    FR3020682B1|2016-05-27|
    WO2015166009A1|2015-11-05|
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    优先权:
    申请号 | 申请日 | 专利标题
    FR1453959A|FR3020682B1|2014-04-30|2014-04-30|METHOD AND SYSTEM FOR DETECTING AT LEAST ONE PARTICLE IN A BODILY LIQUID, AND ASSOCIATED METHOD FOR DIAGNOSING MENINGITIS|FR1453959A| FR3020682B1|2014-04-30|2014-04-30|METHOD AND SYSTEM FOR DETECTING AT LEAST ONE PARTICLE IN A BODILY LIQUID, AND ASSOCIATED METHOD FOR DIAGNOSING MENINGITIS|
    US15/307,539| US9970858B2|2014-04-30|2015-04-29|Method and system for detecting at least one particle in a bodily fluid, and associated method for diagnosing meningitis|
    EP15720071.8A| EP3137874B8|2014-04-30|2015-04-29|Method for diagnosing meningitis|
    PCT/EP2015/059423| WO2015166009A1|2014-04-30|2015-04-29|Method and system for detecting at least one particle in a bodily fluid, and associated method for diagnosing meningitis|
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