Abstract:
The invention relates to an incoherent light full field interference microscopy device for the imaging of a volumetric scattering sample (106). The device comprises an interference device (100) between a reference wave (401), produced by reflection of an incident wave by a reflective surface (105) of a reference arm of the interference device, and an object wave (402) produced by backscattering of the incident wave by a slice of the sample, an acquisition device (108) for at least a first interference signal and at least a second interference signal resulting from the interference of the reference and object waves, the at least two interference signals having a phase difference, an processing unit (403) for calculating an image of the slice of the sample, based on said interference signals. The interference device also comprises an optical element (404) for modifying the phase of the wavefront, and the microscopy device comprises a control unit (405) for the optical element, linked to the processing unit (403), the optical phase modification element being controlled by optimizing a statistical parameter of at least a part of the image calculated by the processing unit.
Abstract:
Procédé d'imagerie par microscopie interfércntielle plein champ d'un échantillon volumique et diffusant placé sur un bras objet d'un dispositif d'interférence. Le procédé comprend une production, au moyen du dispositif d' interférence (200), d'un signal interférométrique bidimensionnel résultant d'une interférence entre, d'une part, une onde de référence obtenue par réflexion d' une onde lumineuse incidente sur une surface de réflexion (205) d'un bras de référence du dispositif d'interférence (200), et, d'autre part, une onde objet obtenue par rétrodiffusion de l 'onde lumineuse incidente par une tranche de cohérence de l'échantillon (206) placé dans le bras objet du dispositif d' interférence (200); une acquisition (320), à différence de marche fixe entre le bras objet et le bras de référence, d'une image interférométrique brute à partir du signal interférométrique bidimensionnel; un calcul (330) d'une image normalisée à partir de l'image interférométrique brute et d'une image de référence; un calcul (340) d'une image OCT plein champ de la tranche de cohérence de l'échantillon par élimination, dans l' image normalisée, de fluctuations spatiales basses fréquences définies en. fonction de la largeur du pic central d'une fonction d'autocorrélation de l 'image interférométrique.
Abstract:
The present invention relates to a full-field optical coherence tomography system (300) for imaging an object (319), comprising a light source (301), a first interferometric device having means for splitting an input light beam and comprising at least a reflecting surface (307), a second interferometric device having means for splitting the spectrally modulated output beam and comprising at least a reflecting surface, a multichannel acquisition device (321), the system (300) being characterized in that at least one of the interferometric devices includes at least a focusing optical element arranged to focus at least one of the input beams or at least one of the output beams onto the corresponding reflecting surface of the corresponding interferometric device.
Abstract:
The present invention relates to a full-field optical coherence tomography system (300) for imaging an object (319), comprising a light source (301), a first interferometric device having means for splitting an input light beam and comprising at least a reflecting surface (307), a second interferometric device having means for splitting the spectrally modulated output beam and comprising at least a reflecting surface, a multichannel acquisition device (321), the system (300) being characterized in that at least one of the interferometric devices includes at least a focusing optical element arranged to focus at least one of the input beams or at least one of the output beams onto the corresponding reflecting surface of the corresponding interferometric device.
Abstract:
Système d'imagerie (20) par microscopie interférentielle plein champ d'un échantillon volumique diffusant (206) comprenant : - un dispositif d'interférence (200) comprenant un bras de référence sur lequel est agencée une surface de réflexion (205), le dispositif d'interférence étant adapté pour produire, lorsque l'échantillon est disposé sur un bras objet du dispositif d'interférence, en chaque point d'un champ d'imagerie, une interférence entre une onde de référence obtenue par réflexion d'ondes lumineuses incidentes sur une surface élémentaire de la surface de réflexion (205) correspondant audit point du champ d'imagerie et une onde objet obtenue par rétrodiffusion d'ondes lumineuses incidentes par un voxel d'une tranche de l'échantillon à une profondeur donnée, ledit voxel correspondant audit point du champ d'imagerie, - un dispositif d'acquisition (208) adapté pour acquérir, à différence de marche fixe entre le bras objet et le bras de référence, une succession temporelle de N signaux interférométriques bidimensionnels résultant des interférences produites en chaque point du champ d'imagerie, - une unité de traitement (220) configurée pour calculer une image (IB, IC) représentative de variations temporelles d'intensité entre lesdits N signaux interférométriques bidimensionnels.
Abstract:
A system that includes an interference device including a reference arm on which a reflective surface is arranged, where the interference device produces, at each point of an imaging field when the sample is placed on a target arm of the interference device, interference between a reference wave and a target wave obtained by backscattering of incident light waves by means of a voxel of a slice of the sample at a given depth; an acquisition device suitable for acquiring, at a fixed path length difference between the target arm and the reference arm, a temporal series of N two-dimensional interferometric signals resulting from the interference produced at each point of the imaging field; and a processing unit that calculates an image representing temporal variations in intensity between said N two-dimensional interferometric signals.
Abstract:
A system that includes an interference device including a reference arm on which a reflective surface is arranged, where the interference device produces, at each point of an imaging field when the sample is placed on a target arm of the interference device, interference between a reference wave and a target wave obtained by backscattering of incident light waves by means of a voxel of a slice of the sample at a given depth; an acquisition device suitable for acquiring, at a fixed path length difference between the target arm and the reference arm, a temporal series of N two-dimensional interferometric signals resulting from the interference produced at each point of the imaging field; and a processing unit that calculates an image representing temporal variations in intensity between said N two-dimensional interferometric signals.
Abstract:
The invention relates to a system (20) for full-field interference microscopy imaging of a three-dimensional diffusing sample (206). Said system includes: an interference device (200) including a reference arm on which a reflective surface (205) is arranged, the interference device being suitable for producing, at each point of an imaging field when the sample is placed on a target arm of the interference device, interference between a reference wave, obtained by reflection of incident light waves onto a basic surface of the reflective surface (205) corresponding to said point of the imaging field, and a target wave obtained by backscattering of incident light waves by means of a voxel of a slice of the sample at a given depth, said voxel corresponding to said point of the imaging field; an acquisition device (208) suitable for acquiring, at a fixed path length difference between the target arm and the reference arm, a temporal series of N two-dimensional interferometric signals resulting from the interference produced at each point of the imaging field; and a processing unit (220) configured to calculate an image (IB, IC) representing temporal variations in intensity between said N two-dimensional interferometric signals.
Abstract:
The present invention relates to a full-field optical coherence tomography system (300) for imaging an object (319), comprising a light source (301), a first interferometric device having means for splitting an input light beam and comprising at least a reflecting surface (307), a second interferometric device having means for splitting the spectrally modulated output beam and comprising at least a reflecting surface, a multichannel acquisition device (321), the system (300) being characterized in that at least one of the interferometric devices includes at least a focusing optical element arranged to focus at least one of the input beams or at least one of the output beams onto the corresponding reflecting surface of the corresponding interferometric device.
Abstract:
The present invention relates to a full-field optical coherence tomography system (300) for imaging an object (319), comprising a light source (301), a first interferometric device having means for splitting an input light beam and comprising at least a reflecting surface (307), a second interferometric device having means for splitting the spectrally modulated output beam and comprising at least a reflecting surface, a multichannel acquisition device (321), the system (300) being characterized in that at least one of the interferometric devices includes at least a focusing optical element arranged to focus at least one of the input beams or at least one of the output beams onto the corresponding reflecting surface of the corresponding interferometric device.