Large numerical aperture imaging device

• US 5,835,265 A
• Filed: 07/18/1996
• Issued: 11/10/1998
• Est. Priority Date: 07/18/1996
• Status: Expired due to Fees

• Current Assignee: Computed Anatomy, Incorporated
• Original Assignee: Computed Anatomy, Incorporated
• Inventors: Mammone, Richard J.
• Primary Examiner(s): NGUYEN, THONG Q
• Application Number:
  US08/683,717
• Time in Patent Office: 845 Days
• Field of Search: 359/362-366, 359/368-369, 359/380, 359/382-385, 359/389, 359/558-559, 359/726-731, 359/850, 359/857-860, 348/75, 348/79-80, 348/207, 348/335-354, 382/128, 382/280, 250/222.1, 250/239, 356/206, 356/347, 356/375
• US Class Current: 359/383
• CPC Class Codes: G02B 21/00 Microscopes
• CPC Class Codes: G02B 21/361 Optical details, e.g. image relay to the camera or image sensor G02B21/364 takes precedence; illumination details G02B21/06 and subgroups
• CPC Class Codes: G02B 21/365 Control or image processing arrangements for digital or video microscopes G02B21/361, G02B21/362 take precedence
• CPC Class Codes: G02B 27/0025 for optical correction, e.g. distorsion, aberration
• CPC Class Codes: G02B 27/46 Systems using spatial filters
• CPC Class Codes: G02B 30/56 by projecting aerial or floating images

Abstract

A microscope having a high effective numerical aperture (NA) is achieved in an apparatus in which a real, three-dimensional image is formed of an object placed in an aperture at the apex of one of two facing, axially-aligned concave mirrors. The three-dimensional image is acquired by a video camera positioned in a counterpart aperture at the apex of the other mirror and the acquired image is processed by computer. The processing corrects the acquired image using the point spread function of the mirror system which was previously obtained by positioning a point source of light throughout the object space and measuring the pixel values recorded by the camera'"'"'s array of sensing element while the camera was positioned at different axial distances in the image space. When the diameter of the mirrors is large compared to the specimen object, substantially all of the light leaving the specimen is captured by the mirrors and focused upon the camera, thereby achieving a high effective numerical aperture for the system which affords excellent resolution, especially when examining transparent specimens.

Claims

1. A large numerical aperture imaging device comprising:

first and second concave mirrors having respective first and second concave reflective surfaces facing each other along an optical axis, each of said surfaces having an aperture at said optical axis, said surfaces being aligned so that most of the light rays from an object placed near the aperture of said first surface are captured at said aperture of said second surface to form a three-dimensional real image thereat, said concave mirrors thereby being used to capture light from said object;

an object support that positions an object at said aperture of said first surface;

an image acquisition device that is mounted for movement along said optical axis at said aperture of said second surface in order to section through said three-dimensional image at various depths along said optical axis thereof, and

means for analyzing the three-dimensional real image acquired by said image acquisition device at said various depths along said optical axis.

2. The imaging device of claim 1 wherein said means for analyzing said image includes a digital computer programmed for processing light intensities existing at said various depths of said acquired three-dimensional image.

3. The imaging device of claim 2 wherein said image acquisition device contains a planar array of sensors for ascertaining said light intensities at said various depths of said acquired three-dimensional image.

4. The imaging device of claim 3 wherein said sensors are selected from the group consisting of charge-coupled devices, metal oxide silicon (MOS) devices, CID devices or vidicon devices.

5. The imaging device of claim 3 wherein said computer includes means for comparing the fast Fourier transform of light intensities from a specimen object imaged at said various depths with the fast Fourier transform of light intensities imaged at said depths by a point source of light positioned at said first-mentioned aperture to obtain the point spread function of said light source.

6. The imaging device of claim 5 wherein said computer is capable of correcting said acquired image for light intensities from the specimen object failing to correspond with the light intensities imaged from said point source.

7. The imaging device of claim 3 wherein said object is a point source of light and wherein said means for analyzing said acquired image includes a computer program for storing the light intensities of said acquired image, received by said image acquisition device in planes perpendicular to the optic axis at each of said various depths.

8. The imaging device of claim 1, further comprising a movable stage, said image acquisition device being mounted on said movable stage, said movable stage being capable of moving said image acquisition device in three dimensions relative to said three-dimensional image.