Method to suppress artifacts in frequency-domain optical coherence tomography

• US 20060171503A1
• Filed: 01/19/2006
• Published: 08/03/2006
• Est. Priority Date: 01/21/2005
• Status: Active Grant

• Current Assignee: Carl Zeiss Meditec Incorporated (Carl-Zeiss-Stiftung)
• Original Assignee: Carl Zeiss Meditec Incorporated (Carl-Zeiss-Stiftung)
• Inventors: O'Hara, Keith E., Hacker, Martin
• Granted Patent: US 7,330,270 B2
• Time in Patent Office: Days
• US Class Current: 378/21
• CPC Class Codes: A61B 5/0066 Optical coherence imaging
• CPC Class Codes: A61B 5/0073 by tomography, i.e. reconstruction of 3D images from 2D projections A61B5/0066 takes precedence
• CPC Class Codes: A61B 5/7257 using Fourier transforms
• CPC Class Codes: G01B 9/0201 using temporal phase variation
• CPC Class Codes: G01B 9/02058 by particular optical compensation or alignment elements, e.g. dispersion compensation
• CPC Class Codes: G01B 9/02078 Caused by ambiguity
• CPC Class Codes: G01B 9/02083 characterised by particular signal processing and presentation
• CPC Class Codes: G01B 9/02091 Tomographic interferometers, e.g. based on optical coherence

Abstract

One embodiment of the present invention is a method for suppressing artifacts in frequency-domain OCT images, which method includes (a) providing sample and reference paths with a significant difference in their chromatic dispersion (b) correcting for the effects of the mismatch in chromatic dispersion, for the purpose of making artifacts in the OCT image readily distinguishable from the desired image.

Claims

1. A method for suppressing artifacts in the image of frequency domain optical coherence tomography, comprising the steps of:

providing a sample path and a reference path that differ in their chromatic dispersion so as to create a variation in relative group delay as a function of optical frequency between the sample and reference paths, wherein the relative group delay variation across the range of optical frequencies recorded is greater than ten times the axial resolution of the optical coherence tomography system;

separating optical radiation from an optical radiation source among the sample path and the reference path;

measuring as a function of optical frequency the combined radiation returned from the sample and reference paths, the measurement producing an interference spectrum;

multiplying the measured interference spectrum by a complex phase factor to compensate for the mismatch in chromatic dispersion; and

processing the compensated interference spectrum to obtain information on the reflectance distribution in the sample path.

2. A method as recited in claim 1, further including the step of positioning a sample to return both optical radiation with optical path length longer than the reference optical path length, and optical radiation with optical path length shorter than the reference optical path length.

3. A method as recited in claim 2, further including the step of repositioning the sample to separate the actual reflectance distribution corresponding to sample features from artifacts of the frequency domain optical coherence tomography measurement.

4. A method as recited in claim 1 further comprising the steps of:

inducing a sequence of different phase shifts in the radiation in at least one of the reference or sample paths;

repeating the measuring and multiplying steps for the different phase shifts; and

processing the results to suppress artifacts in the image.

5. A method as recited in claim 4, wherein said processing step includes generating a linear combination of the measurements at the different induced phase shifts, said combination including coefficients selected to best estimate the actual phase shift occurring between the sample and reference paths.

6. A method as recited in claim 5, wherein the coefficients are selected to maximize image contrast between reflection distribution from the sample and the artifacts.

7. A method for suppressing artifacts in the image of frequency domain optical coherence tomography, comprising the steps of:

providing a sample path and a reference path that differ in their chromatic dispersion so as to create a relative group delay variation as a function of optical frequency between the sample and reference paths;

separating optical radiation from an optical radiation source among the sample path and the reference path;

positioning a sample to return both optical radiation with optical path length longer than the reference optical path length, and optical radiation with optical path length shorter than the reference optical path length;

measuring as a function of optical frequency the combined radiation returned from the sample and reference paths, the measurement producing an interference spectrum;

processing the measured interference spectrum to compensate for the mismatch in chromatic dispersion and using the compensated interference spectrum to obtain information on the reflectance distribution in the sample path;

generating an image based on the information on the reflectance distribution to allow the actual reflectance distribution corresponding to sample features to be distinguished from artifacts of the frequency domain optical coherence tomography measurement; and

repositioning the sample to separate the image of the actual sample features from the artifacts of the frequency domain optical coherence tomography measurement.

8. The method of claim 7, wherein the measuring and processing steps are repeated at several transversely separated locations on the sample to generate data which can be used to form a cross-sectional image of the sample.

9. The method of claim 7, wherein the relative group delay variation across the range of optical frequencies recorded is greater than ten times the axial resolution of the optical coherence tomography system.

10. The method of claim 7, wherein the difference in chromatic dispersion in the paths is created by use of different optical materials in the sample and reference paths.

11. The method of claim 7, wherein the difference in chromatic dispersion in the paths is created by use of one or more dispersive optical elements in the sample or reference paths.

12. The method of claim 7, wherein the interference spectrum is measured with an optical spectrometer.

13. The method of claim 7, wherein the interference spectrum is measured by varying the optical frequency of the optical radiation source.

14. The method of claim 7, wherein the optical coherence tomography is performed with a portion of a human eye as the sample.

15. The method of claim 7, wherein the optical coherence tomography is performed with the sample path routed through an endoscope, and wherein an interior part of the human body is the sample.

16. The method of claim 7, wherein the optical coherence tomography is performed with a section of human skin as the sample.

17. A method as recited in claim 7, wherein said processing step includes multiplying the measured interference spectrum by a complex phase factor to compensate for the mismatch in chromatic dispersion.

18. A method for suppressing artifacts in frequency domain optical coherence tomography comprising the steps of:

providing a sample path and a reference path that differ in their chromatic dispersion so as to create a relative group delay variation as a function of optical frequency between the sample and reference paths;

separating optical radiation from an optical radiation source among the sample path and the reference path;

measuring at a sequence of discrete optical frequencies the combined radiation returned from the sample and reference paths, the measurements producing an interference spectrum, wherein the measurements are taken with non-uniform spacing in optical frequency; and

processing the resulting interference spectrum to obtain information on the reflectance distribution in the sample path wherein the difference in chromatic dispersion is chosen such that a reflection site at a chosen depth in the sample path produces interference fringes that are uniformly spaced in the sequence of discrete optical frequencies used for the measurements.