US2009161203A1PendingUtilityA1

Method and Configuration for the Optical Detection of an Illuminated Specimen

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Assignee: KEMPE MICHAELPriority: Nov 26, 2007Filed: Nov 25, 2008Published: Jun 25, 2009
Est. expiryNov 26, 2027(~1.4 yrs left)· nominal 20-yr term from priority
G02B 27/0031G02B 21/0032G01B 11/24G01B 9/04G02B 26/127G02B 21/0036
49
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Claims

Abstract

A method and a configuration for the depth-resolved optical detection of a specimen, wherein a specimen or a part of the specimen is scanned by means of preferably linear illumination, the illumination of the specimen is periodically structured in the focus in at least one spatial direction, light coming from the specimen is detected and images of the specimen are generated, and at least one optical sectional image and/or one image with enhanced resolution is calculated through the specimen is calculated [sic], images are repeatedly acquired and sectional images are repeatedly blended while changing the orientation of the linear illumination relative to the specimen and/or spatial intervals between from lines exposed to detection light from the illuminated specimen region are generated for the line-by-line non-descanned detection on an area detector or a camera and/or, during a scan, light is further deflected upstream of the detector through the line in the direction of the scan of the specimen.

Claims

exact text as granted — not AI-modified
1 . A method for the depth-resolved optical detection of a specimen, wherein a specimen or a part of the specimen is scanned by means of linear illumination,
 the illumination of the specimen is periodically structured in the focus in at least one spatial direction,   light coming from the specimen is detected and images of the specimen are generated,   and at least one optical sectional image and/or one image with enhanced resolution is calculated through the specimen is calculated [sic],   characterized in that   images are repeatedly acquired and sectional images are repeatedly blended while changing the orientation of the linear illumination relative to the specimen.   
   
   
       2 . The method as in one of the preceding claims [sic], wherein the line is rotated about the optical axis and the images are generated and the sectional images are blended at different angles of rotation. 
   
   
       3 . The method as in one of the preceding claims, wherein, to generate lines, a beam-shaping unit is jointly rotated with means for structuring the illuminating light. 
   
   
       4 . A method for the depth-resolved optical detection of a specimen, wherein a specimen or a part of the specimen is scanned by means of preferably linear illumination,
 the illumination of the specimen is periodically structured in the focus in at least one spatial direction,   light coming from the specimen is detected and images of the specimen are generated,   and at least one optical sectional image and/or one image with enhanced resolution is calculated through the specimen is calculated [sic], in particular as in one of the preceding claims,   
     characterized in that spatial intervals between lines exposed to detection light from the illuminated specimen region are generated for the line-by-line non-descanned detection on an area detector or a camera. 
   
   
       5 . The method as in one of the preceding claims, wherein during the preferably linear illumination and detection, the illumination is repeatedly switched on and off. 
   
   
       6 . The method as in one of the preceding claims, wherein during the scanning of the specimen, the light is repeatedly interrupted so that a spatial interval is formed between two illuminated specimen regions. 
   
   
       7 . The method as in one of the preceding claims for the confocal generation of images, wherein an image is calculated by partially or completely masking the spatial intervals between camera regions associated with the exposed specimen regions and the images thus obtained are blended. 
   
   
       8 . The method as in  claim 7 , wherein the images are blended in such a manner that neighboring scanned regions of the specimen are properly scaled and adjacently aligned in the blended image. 
   
   
       9 . A method for the depth-resolved optical detection of a specimen, wherein a specimen or a part of a specimen is scanned by means of preferably linear illumination,
 the illumination of the specimen is periodically structured in the focus in at least one spatial direction,   light coming from the specimen is detected and images of the specimen are generated,   and at least one optical sectional image and/or one image with enhanced resolution is calculated through the specimen is calculated [sic], in particular as in one of the preceding claims, wherein, during a scanning procedure, light is further deflected upstream of the detector through the line in the direction of the scan of the specimen.   
   
   
       10 . The method as in one of the preceding claims, wherein the speed of the light deflection is greater than the speed of the relative movement between the specimen and the illuminating light. 
   
   
       11 . The method as in one of the preceding claims, wherein the light is deflected step-by-step. 
   
   
       12 . The method as in one of the preceding claims, wherein the light is deflected continuously. 
   
   
       13 . The method as in one of the preceding claims, wherein, during a rotation of the illuminating line, the polarization of the illuminating light is synchronously rotated with the rotation. 
   
   
       14 . The method as in one of the preceding claims, wherein repeated scanning takes place and the position of the periodic structure on the specimen and/or the position of the illuminating light on the specimen is shifted. 
   
   
       15 . The method as in one of the preceding claims, wherein several images with different image phases are acquired and sectional images are calculated therefrom. 
   
   
       16 . The method as in one of the preceding claims, wherein the images are acquired with different image phases with a constant spatial interval between illuminated/detected sections. 
   
   
       17 . The method as in one of the preceding claims, wherein the position of the spatial interval is changed and several images with different image phases are acquired for each position and sectional images are calculated therefrom. 
   
   
       18 . The method as in one of the preceding claims, wherein first the position of the spatial interval for one position of the structure is changed and specimen images are acquired, and subsequently this procedure is repeated for the next position of the structure. 
   
   
       19 . The method as in one of the preceding claims, wherein the position of the spatial interval is changed in such a manner that substantially all specimen regions are sequentially illuminated line-by-line and the specimen light is detected. 
   
   
       20 . The method as in one of the preceding claims, wherein the light is interrupted by decreasing the intensity by means of an electro-optical and/or acousto-optical modulator. 
   
   
       21 . The method as in one of the preceding claims, wherein, for the purpose of the periodic structuring of the illumination, a light beam is divided into several component light beams, which light beams are interferometrically overlapped and shaped into a line. 
   
   
       22 . The method as in one of the preceding claims, wherein the light resulting from a nonlinear interaction of the illumination with the specimen or a part of the specimen . . . [word or words missing] and is detected. 
   
   
       23 . The method as in one of the preceding claims, characterized in that linear scanning is carried out simultaneously with several lines. 
   
   
       24 . The method as in one of the preceding claims, characterized in that the optical section thickness or optical resolution is varied as structures with different modulation frequencies are imaged. 
   
   
       25 . The method as in one of the preceding claims, characterized in that during illumination with several wavelengths, the section thickness is identically set by adjusting each modulation frequency. 
   
   
       26 . A configuration for the depth-resolved optical detection of a specimen, comprising
 means for the preferably linear illumination of the specimen with at least one wavelength,   means for spatially structuring the illuminating light in at least one plane,   means for generating a relative movement between the specimen and the illuminating light,   means for imaging the light influenced by the specimen on at least one detector, and   means for calculating at least one optical sectional image and/or one image with enhanced resolution from the spatial information of the light influenced by the specimen, characterized in that means for changing the orientation of the linear illumination relative to the specimen are provided.   
   
   
       27 . The configuration as in  claim 26 , wherein a jointly rotatable unit comprising a beam-shaping unit to generate lines and means for structuring the illuminating light in the beam path is provided. 
   
   
       28 . A configuration for the depth-resolved optical detection of a specimen, comprising
 means for the preferably linear illumination of the specimen with at least one wavelength,   means for spatially structuring the illuminating light in at least one plane,   means for generating a relative movement between the specimen and the illuminating light,   means for imaging the light influenced by the specimen on at least one detector, and   means for calculating at least one optical sectional image and/or one image with enhanced resolution from the spatial information of the light influenced by the specimen, in particular as in one of the preceding claims, wherein an area detector or a camera for the non-descanned detection of the specimen light is provided and wherein means for interrupting the light during the scan are provided so as to generate a spatial interval between illuminated specimen regions and/or to generate spatial intervals between lines exposed with detection line from the illuminated specimen region on the area detector.   
   
   
       29 . The configuration as in  claim 28 , wherein intensity control means are disposed in the illuminating beam path. 
   
   
       30 . The configuration as in  claim 28  or  29 , wherein an electro- or acousto-optical modulator for light interruption is provided. 
   
   
       31 . A configuration for the depth-resolved optical detection of a specimen, comprising
 means for the preferably linear illumination of the specimen with at least one wavelength,   means for spatially structuring the illuminating light in at least one plane,   means for generating a relative movement between the specimen and the illuminating light,   means for imaging the light influenced by the specimen on at least one detector, and   means for calculating at least one optical sectional image and/or one image with enhanced resolution from the spatial information of the light influenced by the specimen, in particular as in one of the preceding claims, wherein a scanner is disposed in the detection beam path in order to expand the specimen light discretely on the detector or continuously on the detector during the line-by-line scan.   
   
   
       32 . The configuration as in one of the preceding claims, characterized in that at least one scanner is provided as a means for generating the relative movement. 
   
   
       33 . The configuration as in one of the preceding claims, characterized in that the means for structuring the illumination is an optical element that is preferably rotatable about the optical axis and that is structured relative to its transparency. 
   
   
       34 . The configuration as in one of the preceding claims [sic], characterized in that, in order to set different image phases of the structure, the position of at least one scanner can be adjusted. 
   
   
       35 . The configuration as in one of the preceding claims, characterized in that, in order to set different frequency structures, gratings of different periodicities that can be rotated into the beam path are provided. 
   
   
       36 . The configuration or the method as in one of the preceding claims, in a microscope, preferably in a laser scanning microscope.

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