• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
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  • 优先权
    • 专利摘要:
    The present invention relates to a Raman scattering microscopy optical apparatus comprising a laser source (10) adapted to emit a laser beam (11) at an excitation wavelength λ, a microscope objective (14) adapted to receive the laser beam (11) and for focusing the laser beam in an image plane of the microscope objective (14), the focused laser beam (21) being for illuminating a sample (20), an optical system adapted to collect a beam Raman scattering optics (22) and detecting means (16, 17) adapted to detect the collected Raman scattering beam (22). More particularly, it is proposed according to the invention, a Raman scattering microscopy apparatus further comprising an adaptive optics system (31, 32, 33) disposed on an optical path of the excitation laser beam (11), on a optical path of the Raman scattering beam (22) or a common optical path of the excitation laser beam (11) and the Raman scattering beam (22).
    公开号:FR3017947A1
    申请号:FR1451597
    申请日:2014-02-27
    公开日:2015-08-28
    发明作者:Bertrand Dutertre；Denis Cattelan；Emmanuel Fretel
    申请人:Horiba Jobin Yvon SAS；
    IPC主号:
    专利说明:

    [0001] The present invention relates to the field of optical microscopy or Raman microspectrometry, for the analysis of materials or biological samples. In Raman microscopy, a sample is illuminated with an excitation beam, which is generally a laser beam, and scattered light is observed at wavelengths different from the wavelength of the excitation laser beam. Raman microscopy differs from conventional microscopy techniques in which reflected light is observed, transmitted or elastically scattered by the sample at the same wavelength as the illumination beam. There are Raman microscopy devices including for example an optical microscope, a laser source, a microscope objective and a spectrometer. The microscope objective focuses the laser beam at a focal point on the sample and forms a scattering beam. The scattering beam comprises on the one hand a so-called elastic scattering component or Rayleigh component, at the wavelength of the excitation laser, and on the other hand a so-called Raman scattering component, at wavelengths different from the excitation laser, which depend on the nature and structure of the sample. The intensity of the Rayleigh scattering is much greater than the intensity of the Raman scattering, the intensity ratio generally being of the order of 106. A wavelength selective filter, for example of the notch filter type, separates the Raman scattering from the Rayleigh scattering, to detect and analyze the spectrum of the Raman scattering beam.
    [0002] Raman microscopy has many applications in microanalysis of materials and biochips analysis, in which a multitude of biological cells are arranged in a matrix on a coverslip. Adaptive optics systems are known whose optical reflection or refraction characteristics can be modified electronically, for example to correct in real time the effects of certain optical disturbances or aberrations. There are adaptive optics systems based on mirrors or micro-mirrors in which micro-actuators can orient or deform the reflective optical surface. There are also adaptive optics systems operating in transmission, for example liquid crystal modulators (SLM or Spatial Light Modulator) that can spatially modulate the components of a beam in intensity, phase and / or polarization . Adaptive optics systems, particularly with deformable mirrors, have been used for many years in astronomy, for example to correct in real time optical aberrations in a telescope. More recently, adaptive optics systems have been implanted in conventional optical microscopes to correct optical aberrations of the microscope itself or certain optical aberrations induced by nonuniformities in the sample. The publication J. Booth "Adaptive optics in microscopy" Phil. Trans. R. Soc. A 2007 365, 2829-843, discloses the implantation of a deformable mirror (DM) in a confocal fluorescence microscope, to correct the deformations induced by the sample.
    [0003] However, it is known that adaptive optics systems pose certain difficulties: they are very complex to use, they require either a wavefront detector or complicated signal processing algorithms. The use of an adaptive optics system generally requires a very complex calibration procedure. Adaptive optics systems themselves bring optical aberrations that must also be compensated. In beam shaping applications, the size of the laser beam must be adapted to the size of the deformable mirror, liquid lenses with adjustable focal length, or the liquid crystal mirror, because the resolution of the figure of diffraction on the sample depends on it. Finally, adaptive optical transmission systems are configured to operate over a fairly wide wavelength range but which does not cover the entire spectral range of ultraviolet (UVB) to near infrared (NIR) which is that of Raman spectrometry. The difficulties in obtaining a satisfactory signal-to-noise ratio in a state-of-the-art Raman micro-spectrometry apparatus are known to those skilled in the art. However any additional optical system necessarily induces losses by reflection or transmission. Some adaptive optics systems such as those with phase modulation have the disadvantage of not being reciprocal: the phase shift induced on the forward path is not compensated by the phase shift of the return path. It is then necessary to place a phase-modulated system on the path of the incident laser beam and another phase-modulated system on the path of the Raman beam, which doubles the difficulties and the cost of the device. Moreover, the Raman signal is particularly sensitive to the optical materials it passes through, the glasses sometimes induce fluorescence or spurious peaks in the spectra that pollute the analysis of a sample.
    [0004] Those skilled in the art are thus generally discouraged from inserting an additional optical system, and in particular a complex adaptive optics system, into the optical path of the excitation laser beam or the Raman scattering beam, this optical system being capable of to further reduce the signal-to-noise ratio of the Raman micro-spectrometry signal.
    [0005] However, in general, it is desirable to improve the brightness, the spatial resolution, the spectral resolution of a Raman scattering microphotometry apparatus, to allow a more precise analysis of the samples or to allow, in the same way as epifluorescence, to obtain Raman mappings (Mapping Raman), on the one hand better resolved spatially, and on the other hand obtained in less long acquisition times thanks to the best densities of power that they bring by limiting the optical aberrations. On the other hand, a Raman microspectrometry apparatus is generally very sensitive to optical misalignment, which may occur with variations in temperature and vibration. There are optical misalignment correction systems based on a plane mirror whose orientation is automatically adjustable according to the intensity of the Raman signal of a reference spectrum. However, such a system does not make it possible to correct all optical alignment defects in real time. In order to overcome the above-mentioned drawback of the state of the art, the present invention proposes a Raman microscopy or Raman microspectrometry apparatus comprising a laser source adapted to emit a laser beam at an excitation wavelength k. a microscope objective adapted to receive the laser beam and to focus the laser beam in an image plane of the microscope objective, the focused laser beam being for illuminating a sample, an optical system adapted to collect a Raman scattering optical beam on the sample and detection means adapted to detect the collected Raman scattering beam and filtering means adapted to receive the diffusion optical beam and to separate the scattering optical beam on the one hand into a Rayleigh scattering beam, and on the other hand in a Raman scattering beam. More particularly, there is provided according to the invention, a Raman microscopy or Raman microspectrometry apparatus further comprising an adaptive optics system disposed on an optical path of the excitation laser beam, in an optical path of the Raman scattering beam or on a common optical path of the excitation laser beam and the Raman scattering optical beam. The invention advantageously makes it possible to improve the spatial resolution (PSF or Point Spread Function) of a Raman microscopy or Raman microspectrometry apparatus and / or to obtain a better signal-to-noise ratio of the Raman scattering signal. The invention also makes it possible to perform a topographic analysis of the sample. According to particular and advantageous aspects of different embodiments: the Raman microscopy or Raman microspectrometry apparatus is of the confocal type and comprises a confocal hole disposed between the microscope objective and the detection means and said optical system adaptive is disposed on the optical path of the Raman scattering beam downstream of the confocal hole; the laser beam is of Gaussian section and the confocal hole of non-circular or angular shape and said adaptive optics system is configured to adapt the section of the laser beam focused on the sample to the shape of the confocal hole, in the plane of the confocal hole; the Raman microscopy or Raman microspectrometry apparatus further comprises a wavefront detector disposed on an optical path of the laser beam reflected by the sample, the wavefront detector being arranged in an optically conjugated plane with the image plane of the microscope objective, the wavefront detector being adapted to detect a position of the sample in the image plane of the microscope objective; said adaptive optics system comprises at least two adaptive mirrors arranged in series on the optical path of the laser beam between the laser source and the microscope objective, said adaptive mirrors each having a variable focal length and being arranged so as to form a a variable transverse magnification adaptive optics or an adaptive adaptive optical system of variable magnification, the adaptive optics configured to change the diameter of the laser beam on the entrance pupil of the microscope objective according to the diameter of the pupil input of the microscope objective and / or depending on the excitation wavelength; said adaptive optics system is disposed between the laser source and the image plane of the microscope objective, the adaptive optics system being configured to spatially modulate the intensity of the laser beam in the image plane of the objective of microscope; said adaptive optics system is configured to dynamically modulate the intensity and / or phase and / or polarization of the laser beam in the image plane of the microscope objective or in the pupil plane of the microscope objective according to the sample analyzed; the Raman scattering microscopy apparatus comprises a Raman spectrometer adapted to receive and measure a Raman scattering beam, said adaptive optical system being arranged on the optical path of the Raman scattering beam between the microscope objective and the spectrometer Raman, and said adaptive optics system being configured to dynamically modulate the intensity and / or the phase and / or the polarization of the Raman scattering beam at the input of the Raman spectrometer, so as to reduce, in the detected Raman signal, the optical aberrations, for example of astigmatism, induced by the Raman spectrometer.
    [0006] The invention also relates to a Raman microscopy or Raman microspectrometry method comprising the following steps: - emission of a laser beam at an excitation wavelength λ; focusing the laser beam in an image plane of a microscope objective, the focused laser beam being intended to illuminate a sample; - collection of an optical beam of diffusion; filtering the diffusion optical beam so as to separate it on the one hand into an elastic scattering beam, or Rayleigh, and on the other hand into a Raman scattering beam or fluorescence beam; - Detection of the collected Raman scattering beam.
    [0007] According to the invention, the method further comprises a step of modifying the optical properties of an adaptive optics system disposed on an optical path of the excitation laser beam, on an optical path of the Raman scattering beam or on a path common optical excitation laser beam and Raman scattering beam, so as to correct any forms of aberrations generated by the coupling between the microscope and the spectrometer. The Raman microscopy or Raman microspectrometry method thus makes it possible to modify the spatial resolution, the brightness, the spatial distribution of the laser beam on the sample and / or the transmission of the detected Raman scattering beam.
    [0008] The invention will find a particularly advantageous application in the apparatus and methods of Raman microspectrometry and / or fluorescence. The present invention also relates to the features which will emerge in the course of the description which follows and which will have to be considered individually or in all their technically possible combinations. This description, given by way of nonlimiting example, will make it easier to understand how the invention can be made with reference to the appended drawings in which: FIG. 1 schematically represents a Raman optical microspectrometry apparatus according to one embodiment of the invention; invention; FIG. 2 diagrammatically represents an adaptive optics system configured to form the image of a Gaussian laser beam on a confocal hole according to one embodiment of the invention; FIG. 3 illustrates an autofocus system in an optical microscopy apparatus according to a particular embodiment of the invention; - Figure 4 schematically shows an adaptive optics system configured to correct the wavefront of the excitation laser beam according to another embodiment of the invention. FIG. 1 schematically represents an optical microscopy apparatus 100 of the Raman microspectrometry apparatus type. The light microscopy apparatus 100 comprises a laser source 10, which is adapted to emit a laser beam 11 at an excitation wavelength λ. The laser source may be selected from a laser diode, a gas laser, a solid state laser, a diode pumped laser. Depending on the material and the type of laser, the emitted wavelength can be located in the far UV (244 nm, 266 nm), in the near UV range (325nm), in the visible range (405, 473, 532, 633, 785 and 830 nm) or in the near infra-red (1064 nm). The laser beam 11 may be continuous or pulse depending on the type of laser source and the desired applications. Advantageously, an optical system 12 is disposed on the optical path of the laser beam 11 between the laser source 10 and a microscope objective 14. The optical system 12 can be used to adapt the size of the laser beam to that of the pupil of the objective through an adaptive optics variable beam expander system to improve spatial resolution at the focal point and move closer to the Airy spot. The optical system 12 can also be used to adapt the shape of the laser beam 11, generally of circular symmetry, to a particular pupil shape, for example circular in the case of a lens or annular lens in the case of a lens Cassegrain type, so as not to lose energy at the entrance of the lens especially in the case of a low-power beam, for example in the UV. The microscope objective 14 receives the laser beam 11 and forms a focused laser beam 21 in an image plane of the microscope objective 14. A sample 20 is placed in the vicinity of the image plane of the microscope objective 14. The beam Focused laser 21 thus illuminates the sample 20 at a point of transverse dimension ideally close to the Airy spot, ie 1.22k / NA where NA represents the numerical aperture of the microscope objective 14. As depicted in FIG. 1, the microscope objective 14 collects a backscattered beam 22 propagating in the opposite direction to the illumination laser beam. An injection-rejection filter 13, for example a dichroic filter of the high-pass type (edge filter) or the band-cutter (notch filter), makes it possible to spatially separate firstly the Rayleigh scattering component, at the wavelength 2 ,, of the excitation laser beam and secondly the Raman scattering component 220, which is at wavelengths different from the wavelength k. The confocal hole is located on the Raman route alone (222). An optical system 15 is disposed on the optical path of the Raman scattering beam 220 between the microscope objective 14 and the confocal hole, to form the image of the focused point on the confocal hole. Another optical system generally forms the image of the confocal hole on the entrance slit of a spectrometer 16. The spectrometer 16 may be of diffractive or dispersive type. The spectrometer 16 spatially separates the Raman scattering beam 220 into different spectral components 221, 223, 223. A detector 17 detects the intensity of one or more spectral components 221, 222, 223 as a function of the wavelength or of the Raman frequency. An analysis system then makes it possible to process and analyze the spectral components 221, 222, 223 to deduce an analysis of the sample 20. In a transmission configuration (not shown), an optical system collects a beam scattered at through the sample and propagating in the direction of the illumination laser beam.
    [0009] Finally, in another configuration, the scattering beam is collected in a direction transverse to the excitation laser beam. Advantageously, a single microscopy or microspectrometry device may be configured to allow both a backscattering and forward scattering and / or transverse scattering measurement.
    [0010] In a manner known moreover, in certain embodiments of scanning microscopy, the microscopy apparatus further comprises means for angular displacement of the laser beam, consisting for example of a scanner with one or two axes, so that that the focused laser beam scans an area on the surface of the sample. The laser scan makes it possible to form a Raman image of microscopic resolution. In other modes of use, the signal is integrated during the scanning of the laser beam to average the Raman signal over an area of the sample. The Raman microscopy apparatus 100 illustrated in FIG. 1 comprises at least one adaptive optics 31, 32 and / or 33.
    [0011] The adaptive optics 31 is disposed between the laser source 10 and the injection-rejection filter 13 in the optical path of the laser beam 11 only. In the example illustrated in FIG. 1, the adaptive optics system 31 is an optical system operating in reflection, for example of the adaptive mirror type.
    [0012] The adaptive optics system 32 is disposed between the injection-rejection filter 13 and the microscope objective 14 on the common optical path of the excitation laser beam 11 and the scattering beam 22. In the example illustrated in FIG. In FIG. 1, the adaptive optics system 32 is an optical system operating in transmission, for example of the spatial light modulator or SLM type.
    [0013] The adaptive optics 33 is disposed between the injection-rejection filter 13 and the spectrometer 16 in the optical path of the Raman scattering beam 220 alone. In the example illustrated in FIG. 1, the adaptive optics system 33 is an optical system operating in reflection, for example of the adaptive mirror type. Adaptive optics systems 31, 32 and 33 may be used independently of one another or in combination, in pairs, or all together. The arrangement, the number and the type of adaptive optics systems on the different optical paths advantageously make it possible to select a function associated with one of the adaptive optics systems or to combine the functions of several adaptive optics systems.
    [0014] An adaptive optics system 31, 32, 33 may be used to correct optical aberrations in the microspectrometry apparatus and / or the sample, depending on the application. We will detail some embodiments, particularly in connection with Figures 2-4.
    [0015] Figure 2 schematically illustrates a first embodiment, wherein an adaptive optics system 33 is disposed in a confocal type Raman microscope. In Raman micro-spectrometry, a generally confocal hole 19 of generally non-circular shape, such as a diamond shape in Raman micro-spectrometry or of hexagonal form in fluorescence microscopy, is generally used. The confocal hole 19 is made in an opaque support. However, the laser beam 11 from the laser source is generally a Gaussian beam of circular section. The Raman scattering beam 220 is also generally sectionally symmetrical about the optical axis. In the prior art, a conventional optical lens or mirror system forms the image of the waist of the Raman beam in the plane of the confocal hole 19 so that the diameter of the laser beam 11 covers the entire surface of the hole. confocal 19. This image formation induces loss of intensity of the laser beam by vignetting on the edges of the confocal hole 19, in the case where the confocality is not sought but only the brightness, the hole being open at the maiximum.
    [0016] According to the first particular and advantageous embodiment, an adaptive optics system 33 is used configured to form the sample analysis image in the plane of the confocal hole in the plane of the confocal hole 19 and to adapt the shape In an exemplary embodiment, the adaptive optics system 33 consists of an adaptive optics mirror located on the Raman scattering path only. This adaptive optics mirror alters the phase or intensity of the incident field to shape the shape of the beam on the hole differently than the shape of the beam from the source. For example, a diamond-shaped energy distribution is generated in certain cases where the hole has the same size as the image at the focusing point 21, which has the advantage of not causing a loss of signal, but with low confocality. In another example, an elliptical energy distribution is generated within the wide open confocal hole that is imaged on the input slot of the spectrometer so as to obtain an energy distribution in the direction of the height. of the slot, without vignetting on the entrance slit of the spectrometer. This first embodiment allows a gain in brightness on the Raman scattering beam and also allows realignment on the hole, although the confocality properties are relatively low. Figure 3 schematically illustrates a variant of a Raman microscopy or microspectrometry apparatus further comprising a self-focusing or autofocusing device. In microscopy apparatuses of the prior art, the auto focus device generally comprises a pinhole or pinhole and a photodiode type sensor. A semitransparent blade or splitter cube transmits a portion of the laser beam to the microscope objective 14 and returns a portion, typically 10%, of the laser beam reflected from the surface of the sample toward the pinhole. The pinhole, for example 100 microns in diameter, is arranged in a plane optically conjugated with the image plane of the microscope objective. The sensor is arranged behind the pinhole camera. A lens focuses the image of the sample surface on the photodiode. The focal length of the lens is defined so as to have sufficient magnification for a good Z-resolution (beam axis) and thus a good accuracy of the auto focus. A micrometric motorized system generally allows a relative axial displacement between the sample and the microscope objective. The sensor detects the intensity of the reflected signal as a function of this axial displacement. The maximum intensity detected by the photodiode indicates the position of the reflective surface of the sample in the image plane of the objective. An autofocus system thus makes it possible to control the relative axial displacement of a sample plate and the acquisition of the reflection signal on the sensor so as to place the sample in the focal plane of the microscope objective. . However, such a device and self-focusing method is not sensitive to the direction of the defocusing, because the intensity of the reflected beam generally decreases symmetrically on both sides of the image plane. At least one round trip around the image plane is necessary.
    [0017] The devices and methods of self-focusing are therefore generally quite slow and sometimes difficult to converge because they require perfect alignment, especially if starting from an initial position of the sample remote from the image plane of the microscope objective. FIG. 3 illustrates a detail of a Raman scattering microscopy apparatus and more particularly a self-focusing device in such a microscopy apparatus. FIG. 3 shows the microscope objective 14, the image plane (or focal plane) P1 of the microscope objective 14, a plane P2 located between the microscope objective and the image plane P1 and a plane P3 located beyond the image plane P1. A beam splitter 23, for example a semitransparent plate having a reflection coefficient of 10% and a transmission coefficient of 90%, transmits the laser beam 11. in the direction of the microscope objective 14 and returns a portion 31 of the laser beam reflected by the surface of the sample towards a wavefront detector 18, for example a detector or a Shack-Hartmann type camera . The analysis of the reflected beam makes it possible, for example, to decompose the signal into Zernike polynomials.
    [0018] We are particularly interested in the second polynomial Z20. When the reflecting surface of the sample is in the image plane P1, a wavefront signal 181 of determined shape, for example flat, is detected. When the reflecting surface of the sample is in the image plane P2, a wavefront signal 182 is detected, which has a curvature with respect to the signal 181. When the reflecting surface of the sample is in the image plane P3 a wavefront signal 183 is detected, which has a different curvature, opposite to the curvature of the waveform signal 182, with respect to the waveform signal 181. The edge detector wave thus makes it possible to detect the position of the sample in the image plane P1 of the microscope objective more accurately and faster. In addition, the analysis of a Zernike mode (the second polynomial Z20) makes it possible to detect a change of orientation of the curvature of the wavefront and thus to detect the direction of the defocusing of the sample with respect to the image map P1. The autofocusing algorithm can then converge faster than with an intensity detector. Alternatively or complementary, other modes of Zernike could be exploited. Thus, the first mode of Zernike can allow to analyze if the sample is inclined. More generally, the use of adaptive optics and a wavefront detector makes it possible to combine Raman spectrometry with a surface topography technique.
    [0019] In another particular and advantageous embodiment, an adaptive optics system is used comprising two adaptive optical components, in transmission or in reflection, for example of the deformable membrane mirror type, or a system of x2 liquid lenses arranged in series on the optical path of the laser beam 11. The two adaptive optical components are arranged to form an afocal adaptive optical system.
    [0020] In this embodiment, the two adaptive optical components are configured to have radii of curvature different from one another, so as to form an adaptive optical system, for example afocal having a magnification other than 1. In a first variant , the adaptive optical system can be modified so that the focal length of one or both mirrors varies, while maintaining an afocal system arrangement, so as to form an afocal optical system of variable magnification, preferably greater than 1 Such afocal adaptive optical system allows different applications. In a first application, an afocal adaptive optical system of variable magnification is disposed on the optical path of the laser beam 11 between the laser source 10 and the microscope objective 14 or on the common path. The two focal lengths of the two adaptive optical components vary together, which makes it possible to adapt the size of the laser to the pupil of each objective at any wavelength. This system allows an improvement of the spatial resolution to reach the diffraction limit (Airy spot).
    [0021] The variable magnification of the adaptive optics system makes it possible to form a variable beam expander. This adaptive optics system makes it possible to adapt the diameter of the laser beam to the pupil diameter of the objective and thus to limit the intensity losses on the excitation laser beam. Such an adaptive adaptive optics system of variable magnification allows a change of excitation laser, for example to change the wavelength k, while optimizing the transfer of intensity from the laser source to the microscope objective. In another variant, the adaptive optical system may be modified so that the focal length of one or both mirrors varies, so as to form a focusing optical system of variable transverse magnification.
    [0022] In another application, the adaptive optical system is only available on the common path. Then, the adaptive optical system is voluntarily disrupted so as to converge on the objective pupil and thereby illuminate a larger area of the sample. This configuration makes it possible to quickly locate areas of interest by matrix camera imaging and to perform a Raman analysis on these areas of interest after a coarse registration.
    [0023] This configuration avoids sweeping the entire surface of the sample to locate an area of interest. In another particular and advantageous embodiment, an adaptive optics system 31 is used arranged on the optical path of the laser beam between the laser source 10 and the microscope objective 14 to modify the spatial energy distribution of the beam focused on In a particularly advantageous manner, particle morphology recognition software (of the "particle finder" software module type optionally supplied with the HORIBA LabSpec6 Raman analysis software) is coupled with an adaptive optics system. to spatially structure the shape of the laser according to the shape of the particle to be analyzed.
    [0024] For example, a spatial light adaptive optical system calculates the Fourier transform of an image, for example an image of the sample with particles, and imposes this hologram on the adaptive optical modulation system. liquid crystal phase. After reflecting the laser beam on this adaptive phase-modulated optical system, the output beam of the adaptive phase-modulated optical system reproduces the initial image (see article Holographic analysis of caged neurotransmitter NATURE METHODS VOL.5 NO.9 SEPTEMBER 2008 ) or better still, re-image the particles illuminated in the direction of the height of the entrance slit of the spectrometer which makes it possible to analyze several particles at the same time by a single CCD reading. The difficulty lies in the fact that a second adaptive optics system is required on the Raman scattering path (the first being on the laser path only) which recombines all the illuminated particles at the same time into the single confocal hole. In fact, a single adaptive optics system with phase modulation on the common path would not work because such an adaptive optics system is not reversible, the phase changed on the outward would be doubled on return and not compensated. . The advantage of this embodiment is to illuminate only the area of interest without illuminating the surroundings, which would be detrimental to the signal / noise ratio. This embodiment makes it possible to avoid undesirable areas on the sample by concentrating the energy of the laser beam only on the useful part of the optical field. This eliminates unwanted signals from surrounding particles or the substrate. In another variant, the adaptive optics system 31 is used to correct the spatial distribution of the laser wavefront so as to reduce the spatial extent of the laser beam at the focal point (or PSF for point spread function) and / or to correct the optical aberrations, in particular from the index variations in the sample itself, so as to improve the spatial resolution of the microscopy apparatus. FIG. 4 illustrates an exemplary wavefront correction of the excitation laser beam. FIG. 4A shows a longitudinal section of the laser beam 11 around the waist, that is to say, the focusing zone. In the absence of deformation of the adaptive optics system 310, the laser beam has disturbances, due to optical aberrations induced by the microscopy apparatus and / or by the sample. FIG. 4B shows the effect of a deformation 311 of the adaptive optics system, which is configured to compensate for the disturbances of the wavefront of the laser beam. The adaptive optics system 31 thus configured makes it possible to eliminate the disturbances of the laser beam (FIG. 4C). This embodiment thus makes it possible to improve the spatial resolution at the point of focus of the laser beam. In another embodiment, there is an adaptive optics system 33 between the filter 13 and the spectrometer 16, in the optical path of the Raman scattering beam 22.
    [0025] Advantageously, the adaptive optics system 33 is configured to compensate for optical aberrations of the spectrometer. Thus we succeed in correcting the defect of astigmatism for example, by modulating the beam as a cylindrical lens which decomposes the sagittal and tangential planes and modifies only one of these planes. A radius of curvature is created in one direction of the adaptive optics mirror without affecting the other. This embodiment makes it possible to create a cylindrical lens with a variable focal length in a single direction to compensate for the amplitude of the astigmatism defect. More particularly, the adaptive optics system 33 is configured to compensate for the astigmatic defect caused by the mirrors of the spectrometer, in order to suppress astigmatism defects on the detector 17 while obtaining a better detected energy density. For example, the adaptive optics system 33 is controlled to induce an inverse astigmatism defect to that of the spectrometer 16 prior to the input slot of the spectrometer. The lines of a spectrum correspond to points imaged on a CCD type detector.
    [0026] For the lines to be fine (good spectral resolution), it is arranged to draw the concave mirrors inside the spectrometer so as to have image points on CCD the finest possible. So we have vertical elliptical points and therefore a loss on height. By making a CCD image of the spot on the detector, this astigmatism defect is very well visualized and partially corrected by placing a cylindrical lens that compensates for this defect before the slot by creating the opposite defect. This embodiment avoids the use of a single passive optics system dedicated to each spectrometer 16. In another embodiment, one or more adaptive optics components are used in a Raman microscopy apparatus for Automatically stabilize the optical alignment of the Raman microscopy instrument with respect to thermal drifts or vibrations but also a stabilization of the sample focus. Thus, a control spectrum with reference sample is acquired under particular conditions to obtain an indication of the general state of the instrument. For highly dispersive systems (which is usually a large, focal length device) subject to dilation, adaptive optics is used to compensate for signal loss without losing the very careful factory alignment. In this case, more than a performance enhancement function, adaptive optics has a role in maintaining the quality of a device.
    权利要求:
    Claims (9)
    [0001]
    REVENDICATIONS1. Raman microscopy or Raman microspectrometry apparatus (100) comprising: - a laser source (10) adapted to emit a laser beam (11) at an excitation wavelength λ 2; a microscope objective (14) adapted to receive the laser beam (11) and to focus the laser beam in an image plane of the microscope objective (14), the focused laser beam (21) being intended to illuminate a sample (20); an optical system (14) adapted to collect a scattering optical beam (22) on the sample; filtering means adapted to receive the diffusion optical beam (22) and to separate the diffusion optical beam (22) on the one hand into a Rayleigh scattering beam, and on the other hand into a Raman scattering beam ( 220); detection means (16, 17) adapted to detect the collected Raman scattering beam (220), characterized in that the Raman microscopy or Raman microspectrometry apparatus (100) further comprises: an optical system adaptive array (31, 32, 33) disposed on an optical path of the laser beam (11), on an optical path of the Raman scattering beam (220) and / or on a common optical path of the laser beam (11) and the optical beam Raman scattering (220).
    [0002]
    Raman microscopy or Raman microspectrometry apparatus according to claim 1, wherein said microscopy apparatus is of confocal type and comprises a confocal hole (19) disposed between the microscope objective (19) and the detection means (16, 17) and wherein said adaptive optics system (31) is disposed on the optical path of the Raman scattering beam (220) downstream of the confocal hole (19).
    [0003]
    3. Raman microscopy or Raman microspectrometry apparatus according to claim 2, wherein the laser beam (11) is of Gaussian section and the confocal hole (19) of non-circular or angular shape, said adaptive optics system (31). is configured to match the section of the focused laser beam on the sample to the shape of the confocal hole (19) in the plane of the confocal hole (19).
    [0004]
    4. Raman microscopy or Raman microspectrometry apparatus according to one of claims 1 to 3, further comprising a wavefront detector (18) disposed on an optical path of the reflected laser beam (31) by the sample (20). ), the wavefront detector (18) being disposed in a plane optically conjugated with the image plane (P1) of the microscope objective (14), the wavefront detector (18) being adapted to detect a position of the sample in an image plane (P1) of the microscope objective (14).
    [0005]
    Raman microscopy or Raman microspectrometry apparatus according to one of claims 1 to 4, wherein said adaptive optics system (31) comprises at least two adaptive mirrors arranged in series on the optical path of the laser beam between the source. laser and the microscope objective, said at least two adaptive mirrors each having a variable focal length and being arranged to form a variable magnification focusing adaptive optical system or an afocal adaptive optical system of variable magnification, the adaptive optical system being configured to change the diameter of the laser beam (11) on the entrance pupil of the microscope objective (14) according to the diameter of the entrance pupil of the microscope objective (14).
    [0006]
    Raman microscopy or Raman microspectrometry apparatus according to one of claims 1 to 5, wherein said adaptive optics system (31, 32) is disposed between the laser source and the image plane of the microscope objective, the adaptive optics system (31) being configured to spatially modulate the intensity of the laser beam (11) in the image plane (P1) of the microscope objective (14).
    [0007]
    The Raman microscopy or Raman microspectrometry apparatus according to claim 6 wherein said adaptive optics system (31, 32) is configured to dynamically modulate the intensity and / or phase of the laser beam (21) in the image plane. of the microscope objective (14) or in the pupil plane of the microscope objective as a function of the sample (20) analyzed.
    [0008]
    Raman microscopy or Raman microspectrometry apparatus according to one of claims 1 to 7, comprising a spectrometer (16, 17) adapted to receive and measure a Raman scattering beam (220), said adaptive optics system (33). being disposed in the optical path of the Raman scattering beam between the microscope objective (14) and the spectrometer (16, 17), and said adaptive optics system (33) being configured to dynamically modulate the intensity and / or the phase of the Raman scattering beam (22) at the input of the spectrometer (16, 17), so as to reduce, in the detected Raman signal, the optical aberrations, for example of astigmatism, induced by the spectrometer (16, 17 ).
    [0009]
    9. Raman microscopy or Raman microspectrometry method comprising the following steps: emission of a laser beam (11) at an excitation wavelength λ 2; focusing the laser beam (11) in an image plane of a microscope objective (14), the focused laser beam (21) being for illuminating a sample (20); collection of a scattering optical beam (22); filtering the scattering optical beam (22) so as to separate it on the one hand into an elastic scattering beam, or Rayleigh beam, and on the other hand into a Raman scattering beam (220) or fluorescence beam; detection of the Raman scattering beam (220) collected, characterized in that it comprises a step of: - modifying the optical properties of an adaptive optics system (31, 32, 33) arranged on an optical path of the laser beam excitation circuit (11), on an optical path of the Raman scattering beam (220) or on a common optical path of the excitation laser beam (11) and the Raman scattering beam (220), so as to modify the spatial resolution, brightness, spatial distribution of the laser beam on the sample (20) and / or transmission of the Raman scattering beam detected.
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    同族专利:
    公开号 | 公开日
    EP3111178B1|2020-11-18|
    US10139346B2|2018-11-27|
    CN106461925A|2017-02-22|
    WO2015128579A1|2015-09-03|
    FR3017947B1|2019-05-24|
    CN106461925B|2020-05-12|
    CN106461925B9|2020-07-07|
    US20160363538A1|2016-12-15|
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    引用文献:
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    US20130278744A1|2010-11-22|2013-10-24|Ecole Polytechnique|Method and system for calibrating a spatial optical modulator in an optical microscope|WO2017148668A3|2016-03-04|2017-10-12|Vg Systems Limited|Xps and raman sample analysis system and method|US20110109903A1|2009-11-09|2011-05-12|National Tsing Hua University|Imaging Spectrometer|
    CN102499630B|2011-11-04|2013-08-21|南京航空航天大学|Adaptive optics technology based living human eye retinal cell microscope|KR20160115682A|2015-03-25|2016-10-06|삼성전자주식회사|Method of enabling spatially varying auto focusing of objects and an image capturing system thereof|
    US20190310451A1|2016-11-10|2019-10-10|The Trustees Of Columbia University In The City Of New York|Rapid High-Resolution Imaging Methods for Large Samples|
    DE102017203492A1|2017-03-03|2018-09-06|Witec Wissenschaftliche Instrumente Und Technologie Gmbh|Method and device for imaging a sample surface|
    CN107037031A|2017-05-23|2017-08-11|北京理工大学|The confocal CARS micro-spectrometers method and device of reflection type differential|
    CN107907512B|2017-10-13|2020-04-07|中国科学院上海技术物理研究所|Deep space exploration micro-area self-adaptive Raman fluorescence imaging combination method|
    CN108693161B|2018-04-11|2021-03-23|中国计量科学研究院|Raman spectrum imaging point spread function detection die body and preparation method and application thereof|
    CN108593620B|2018-05-28|2021-02-26|中国计量大学|Multicolor super-resolution imaging system applied to 4pi microscopic framework|
    CN110567959A|2019-09-17|2019-12-13|哈工大机器人无人装备与人工智能研究院|Self-adaptive aberration correction image scanning microscopic imaging method and device|
    CN110596877A|2019-09-17|2019-12-20|四川大学|Optical zoom microscope with continuously adjustable focal lengths of objective lens and ocular lens|
    法律状态:
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    优先权:
    申请号 | 申请日 | 专利标题
    FR1451597|2014-02-27|
    FR1451597A|FR3017947B1|2014-02-27|2014-02-27|SYSTEM AND METHOD FOR OPTICAL ADAPTIVE OPTICAL RAMAN DIFFUSION MICROSCOPY|FR1451597A| FR3017947B1|2014-02-27|2014-02-27|SYSTEM AND METHOD FOR OPTICAL ADAPTIVE OPTICAL RAMAN DIFFUSION MICROSCOPY|
    PCT/FR2015/050447| WO2015128579A1|2014-02-27|2015-02-24|Optical microscopy system and method for raman scattering with adapative optics|
    CN201580023009.7A| CN106461925B9|2014-02-27|2015-02-24|System and method for Raman scattering optical microscope with adaptive optics system|
    EP15715783.5A| EP3111178B1|2014-02-27|2015-02-24|Optical microscopy system and method for raman scattering with adaptive optics|
    US15/121,632| US10139346B2|2014-02-27|2015-02-24|Optical microscopy system and method for Raman scattering with adaptive optics|
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