Methods and systems for reducing complex conjugate ambiguity in interferometric data
AssigneeDuke University
InventorsMichael Choma, Joseph A. Izatt, Anjul Davis
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AssigneeDuke University
InventorsMichael Choma, Joseph A. Izatt, Anjul Davis
Estimating the term…
A complex conjugate ambiguity can be resolved in an Optical Coherence Tomography (OCT) interferogram. A reference light signal is propagated along a reference path. A sample light signal is impinged on a sample reflector. The reference light signal is frequency shifted with respect to the sample light signal to thereby separate a positive and a negative displacement of a complex conjugate component of the OCT interferogram.
A method for resolving a complex conjugate ambiguity in an Optical Coherence Tomography (OCT) interferogram, the method comprising:
A interferometry system for resolving a complex conjugate ambiguity in an Optical Coherence Tomography (OCT) interferogram, the system comprising:
Dependencies are inferred from the claim text.
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Using two or more frequencies: using frequency scans
Characterised by controlling or generating intrinsic radiation properties: using two or more frequencies
By electronic control systems, i.e. using feedback acting on optics or light: synchronization of light source or manipulator and detector
Of particular errors: caused by ambiguity
Term ended 17 Aug 2026 (estimated)
The present invention relates to methods and systems for imaging, and more particularly, to the reduction of image artifacts.
Since its introduction in the early 1990's, optical coherence tomography (OCT) has emerged as a promising imaging modality for micrometer-scale noninvasive imaging in biological and biomedical applications. Its relatively low cost and real-time, in vivo capabilities have fueled the investigation of this technique for applications in retinal and anterior segment imaging in ophthalmology (e.g., to detect retinal pathologies), early cancer detection and staging in the skin, gastrointestinal, and genitourinary tracts, as well as for ultra-high resolution imaging of entire animals in embryology and developmental biology. Conventional OCT systems are essentially range-gated low-coherence interferometers that have been configured for characterization of the scattering properties of biological and other samples. By measuring singly backscattered light as a function of depth, OCT fills a valuable niche in imaging of tissue ultrastructure, and provides subsurface imaging with high spatial resolution (˜5-10 μm) in three dimensions and high sensitivity (>110 dB) in vivo with no contact needed between the probe and the tissue. OCT is based on the one-dimensional technique of optical coherence domain reflectometry (OCDR), also called optical low-coherence reflectometry (OLCR). See Youngquist, R. C., S. Carr, and D. E. N. Davies, Optical Coherence Domain Reflectometry: A New Optical Evaluation Technique. Opt. Lett., 1987. 12: p. 158; Takada, K., et al., New measurement system for fault location in optical waveguide devices based on an interferometric technique. Applied Optics, 1987. 26(9): p. 1603-1606; and Danielson, B. L. and C. D. Whittenberg, Guided-wave Reflectometry with Micrometer Resolution. Applied Optics, 1987. 26(14): p. 2836-2842. In some instances of time-domain OCT, depth in the sample is gated by low coherence interferometry. The sample is placed in the sample arm of a Michelson interferometer, and a scanning optical delay line is located in the reference arm.
The time-domain approach used in conventional OCT may be used in supporting biological and medical applications. An alternate approach involves acquiring the interferometric signal generated by mixing sample light with reference light at a fixed group delay as a function of optical wavenumber. Two methods have been developed which employ this Fourier domain (FD) approach. The first is generally referred to as Spectral-domain OCT (SDOCT). SDOCT uses a broadband light source and achieves spectral discrimination with a dispersive spectrometer in the detector arm. The second is generally referred to as swept-source OCT (SSOCT). SSOCT time-encodes wavenumber by rapidly tuning a narrowband source through a broad optical bandwidth. Both of these techniques can provide improvements in SNR of up to 15-20 dB when compared to time-domain OCT, because SDOCT and SSOCT capture the complex reflectivity profile (the magnitude of which is generally referred to as the “A-scan” data or depth-resolved sample reflectivity profile) in parallel. This is in contrast to time-domain OCT, where destructive interference is employed to isolate the interferometric signal from only one depth at a time as the reference delay is scanned.
FIG. 1 is a flowchart illustrating operations according to embodiments of the present invention.
FIG. 2 is a schematic diagram of optical systems and methods according to embodiments of the present invention including a swept source interferometer and a Doppler shifted reference arm.
FIG. 3 is a schematic diagram of optical systems and methods according to embodiments of the present invention in which data is acquired evenly spaced in wavenumber (k).
The present invention now will be described hereinafter with reference to the accompanying drawings and examples, in which embodiments of the invention are shown. This invention may, however, be embodied in many different forms and should not be construed as limited to the embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete, and will fully convey the scope of the invention to those skilled in the art.
The terminology used herein is for the purpose of describing particular embodiments only and is not intended to be limiting of the invention. As used herein, the singular forms “a”, “an” and “the” are intended to include the plural forms as well, unless the context clearly indicates otherwise. It will be further understood that the terms “comprises” and/or “comprising,” when used in this specification, specify the presence of stated features, integers, steps, operations, elements, and/or components, but do not preclude the presence or addition of one or more other features, integers, steps, operations, elements, components, and/or groups thereof.
It will be understood that, although the terms first, second, etc. may be used herein to describe various elements, components, regions, layers and/or sections, these elements, components, regions, layers and/or sections should not be limited by these terms. These terms are only used to distinguish one element, component, region, layer or section from another region, layer or section. Thus, a first element, component, region, layer or section discussed below could be termed a second element, component, region, layer or section without departing from the teachings of the present invention.