Phase Sensitive Fourier Domain Optical Coherence Tomography

• US 20090015842A1
• Filed: 03/21/2005
• Published: 01/15/2009
• Est. Priority Date: 03/21/2005
• Status: Abandoned Application

• Current Assignee: Ecole polytechnique fãdãrale de lausanne epfl (Schweizerische Eidgenossenschaft)
• Original Assignee: Ecole polytechnique fãdãrale de lausanne epfl (Schweizerische Eidgenossenschaft)
• Inventors: Lasser, Theo, Bachmann, Adrian, Leitgeb, Rainer
• Application Number:
  US11/886,592
• Publication Number:
  US 20090015842A1
• Time in Patent Office: Days
• US Class Current: 356/456
• 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 2290/45 Multiple detectors for detecting interferometer signals
• CPC Class Codes: G01B 2290/70 Using polarization in the interferometer
• CPC Class Codes: G01B 9/02003 using beat frequencies
• CPC Class Codes: G01B 9/02044 Imaging in the frequency domain, e.g. by using a spectrometer
• CPC Class Codes: G01B 9/02069 Synchronization of light source or manipulator and detector
• CPC Class Codes: G01B 9/02091 Tomographic interferometers, e.g. based on optical coherence

Abstract

Optical Coherence Tomography (OCT) is an imaging technique with high axial resolution in the micro-meter-scale range combined with a high sensitivity allowing for example to probe weakly back-scattering structures beneath the surface of biological tissues up to several millimeters. A major improvement of this conventional technique represents Fourier Domain OCT with a further decrease in image acquisition time and additional sensitivity. The apparatus including appropriate signal processing reconstructs the depth profile from the spectrally resolved light signal generated by a broadband source and an interferometric imaging system. By frequency shifting the light fields with frequency shifting means in the reference and sample arm a phase resolved signal at high speed can be registered. Therefore the reference arm does not rely on arm length changes or delays. The beating signal generated in this way shows high phase stability. The phase of this beating signal is not wavelength dependent, as the frequency shift applied is the same for all wavelengths. Moreover this results in an additional suppression of unwanted auto-correlated distortion as well as an extended depth range.

Claims

1. An optical system for phase-resolved, Fourier domain optical coherence tomography, comprising

a) a source

b) an interferometer comprising optical means for splitting and recombining the different light fields, the means for splitting light fields defining an optical sample path (sample arm) providing a sample arm light with a region of illumination on the sample and an optical reference path (reference arm) providing a reference arm light,

c) at least one frequency shifting mean for generating a wavelength independent beating signal at the detector,

d) a pre-adjusted, but fixed reference arm length during the measurement,

e) a synchronization unit,

f) at least one spectrometer combined with at least one detector for recording at least one spectrum at a given time point,

g) a data processor for processing the detected optical signals and delivering a tomogram,

wherein the at least one frequency shifting mean and the at least one detector are synchronized by the synchronization unit resulting in a wavelength independent, phase-resolved measurement.

2. An optical system according to claim 1, wherein at least three frequency shifting means for generating appropriate beat frequencies

a) for measuring only the autocorrelation contribution resulting from light interactions in the reference arm,

b) for measuring only the autocorrelation contribution resulting from interactions in the sample arm including light sample interactions

c) or for measuring the cross-correlation between both arms

by an appropriate synchronisation of the clock frequency of at least one of the detectors to the specific beat frequencies.

3. An optical system according to claim 1, wherein the optical means for guiding, splitting and recombining the different light fields are selected from the group comprising “

free space optical beam splitters and circulators”

or are selected from the group comprising fiberoptical elements as fiberoptic 2×

2 wave couplers, fiberoptic 1×

2 and 2×

1 wave couplers, optical circulators or combinations of free space optical elements with fiberoptical elements.

4. An optical system according to claim 1, wherein the at least one frequency shifting mean is selected from the group comprising acousto-optic frequency shifting means or mechanical frequency shifting elements.

5. An optical system according to claim 1, wherein frequency shifting means are provided in the sample and/or the reference arm.

6. An optical system according to claim 1, wherein the interferometer contains more than one reference and/or more than one sample arm and/or is combined with optionally a multitude of additional interferometers, where these interferometers may be of a different and/or a multitude of different interferometer types.

7. An optical system according to claim 1, wherein more than one frequency shifting means are provided in the same arm.

8. An optical system according to claim 1, wherein the at least one detector is selected from the group comprising line detectors, 1D or multi-dimensional array detectors.

9. An optical system according to claim 1, wherein the at least one detector is selected from the group comprising array detector with an on chip integrated signal processing electronics for measuring an oscillatory component.

10. An optical system according to claim 1, wherein the synchronization unit locks the clock frequency or a multiple of the clock frequency of the detector to the frequency difference of the frequency shifting means.

11. An optical system according to claim 1 additionally comprising a scanning unit for displacing the light fields on the sample and redirecting reflected light components back into the interferometer.

12. An optical system according to claim 11, wherein the scanning unit comprises a unit for displacing the sample in at least one dimension within the sample space.

13. An optical system according to claim 1 additionally comprising components for dispersion compensation in the reference arm and/or sample arm.

14. An optical system according to claim 1 additionally comprising polarization-sensitive optical elements and/or polarization-controlling optical elements in the sample and/or the reference arm, enabling the detection of spectra for at least two different states of polarization.

15. An optical system according to claim 14, wherein two or more spectra at different states of polarization are detected using one or more spectrometers, each equipped with at least one detector.

16. An optical system according to claim 1, wherein the detected optical signals are processed by the data processor using an algorithm from the group of Fourier-transform based algorithms for calculating the depth profile and/or deduced phase or amplitude information from the measured spectra.

17. An optical system according to claim 1, wherein a plurality of spots on the sample are illuminated simultaneously.

18. An optical system according to claim 1, wherein a region in the geometrical form of a continuous line on the sample is illuminated simultaneously.

19. An optical system according to claim 1, wherein the light field of the optical sample path is reflected from the region of illumination on the sample and detected by the at least one detector.

20. An optical system according to claim 1 wherein light of the light field of the optical sample path with a region of illumination on the sample is transmitted through the sample and detected by the at least one detector.

21. An optical system according to claim 1, wherein “

the optical paths are configured as free-space optics”

.

22. An optical system according to claim 1, wherein “

the optical paths are configured as fiber-optical paths”

.

23. An optical system according to claim 22 comprising polarization maintaining fibers and wave couplers.

24. An optical system according to claim 1, additionally comprising beam shaping optical components.

25. An optical system according to claim 1 combined with an interferometric source comprising at least one frequency shifting mean.

27. The use of an optical system according to claim 1 for, but in no case limited to

a) polarization sensitive measurements

b) absorption measurements

c) spectroscopic property measurements

d) differential phase measurements

e) static or dynamic dispersion measurements

f) measurements of functional parameters as blood flow, tissue elasticity, tissue properties etc.

g) measurement of defect localization in transparent or semitransparent media

h) measurement of spectroscopic defect characteristics if transparent or semitransparent media

of technical and/or biological samples.

26. An optical system comprising a common path interferometer combined with an interferometric source comprising at least one frequency shifting mean.