Method and apparatus for three-dimensional imaging using laser illumination interferometry

• US 5,926,277 A
• Filed: 11/25/1998
• Issued: 07/20/1999
• Est. Priority Date: 09/08/1987
• Status: Expired due to Term

• Current Assignee: Coherix Incorporated
• Original Assignee: ERIM International, Inc. (Altarum Institute)
• Inventors: Marron, Joseph C., Gleichman, Kurt W.
• Primary Examiner(s): Kim, Robert H.
• Application Number:
  US09/199,629
• Time in Patent Office: 237 Days
• Field of Search: 356/345, 356/359, 356/360, 356/346
• US Class Current: 356/512
• CPC Class Codes: G01B 11/2441 using interferometry
• CPC Class Codes: G03H 1/0443 Digital holography, i.e. recording holograms with digital recording means holobject computation G03H1/0866
• CPC Class Codes: G03H 1/0866 Digital holographic imaging, i.e. synthesizing holobjects from holograms
• CPC Class Codes: G03H 2001/0458 Temporal or spatial phase shifting, e.g. parallel phase shifting method
• CPC Class Codes: G03H 2222/13 Multi-wavelengths wave with discontinuous wavelength ranges G03H2222/18 takes precedence

Abstract

A method for determining a range dimension of an object utilizing multiple wavelength interferometry to form an image of the object includes developing a discernible two-dimensional image from an interference pattern at selected points for each of a number of wavelengths, collecting complex values from the interference pattern and developing a phase value from the complex value, and determining a phase correction vector based on a difference between measured phase values and an ideal phase value associated with one or more reference points. The phase correction vector is used to correct each of the selected points. A one-dimensional Fourier transform is performed on the corrected values to yield a range profile for each selected point. A peak value is then determined from the range profile to determine the range dimension. The peak value may be determined based on a simple maximum, oversampling in selected areas prior to performing the Fourier transform, or using curve-fitting techniques. The phase correction vector minimizes phase errors due to various causes such as insufficient knowledge of the laser frequencies, or which occur when optical path lengths of the object and reference beams are not match, to provide a computationally efficient method of improving accuracy in the range dimension.

Claims

1. In a method of forming an image of an object utilizing multiple wavelength interferometry, a method for determining the range dimension of the object, the method comprising:

developing a two-dimensional representation of the image of the object from an interference pattern for each of a plurality of wavelengths at each of a plurality of selected points on the object;

developing a complex value from the two-dimensional representation of the image for each of the plurality of wavelengths at each of the plurality of selected points on the object;

performing a one-dimensional Fourier transform on a series of the complex values for each of the selected points to yield a range profile for each selected point; and

determining a peak value for each of the range profiles to determine the range dimension of the object.

2. The method of claim 1 wherein the peak value is determined by:

locating a likely peak on the range profile;

oversampling the one-dimensional Fourier transform in an area proximate to the likely peak; and

locating a peak value from the range profile of the area.

3. The method of claim 1 wherein the peak value is determined by:

locating a likely peak on the range profile;

curve-fitting the range profile near the likely peak; and

determining a peak value based on the curve-fitting.

4. The method of claim 1 further including constructing a three-dimensional image of the object at the selected points based upon the peak value for each of the range profiles.

5. The method of claim 1 further comprising applying a phase correction vector to the complex value prior to performing the one-dimensional Fourier transform.

6. The method of claim 5 wherein applying a phase correction vector comprises:

selecting at least one reference point on the object;

determining a difference between each measured phase value and an associated ideal phase value for each of the wavelengths at the at least one reference point;

establishing a phase correction vector from the differences;

establishing corresponding corrected values for points associated with the at least one reference point by adding the phase correction vector to the complex value of each point; and

replacing the complex value with the corresponding corrected value for each of the points associated with the reference point.

7. The method of claim 6 wherein the step of selecting at least one reference point comprises:

selecting a temporary reference point;

defining a neighborhood of points surrounding and including the temporary reference point;

comparing data from selected wavelengths for each point in the neighborhood to determine the point having superior phase information data; and

replacing the temporary reference point with the point having superior phase information based on the step of comparing.

8. The method of claim 7 wherein the neighborhood comprises nine pixels.

9. The method of claim 6 wherein the points associated with a reference point form a subset of the selected points.

10. The method of claim 6 wherein at least two reference points are selected.

11. The method of claim 5 wherein the phase correction vector is a complex conjugate of the difference between each measured phase value and the associated ideal phase value for each of the wavelengths at the at least one reference point.

12. The method of claim 1 wherein the two-dimensional representation of the object is a discernible two-dimensional image obtained by utilizing a lens to perform a two-dimensional transform of the interference pattern while focusing the interference pattern on a two-dimensional detector array which is positioned in the image plane of the lens.