Processes, arrangements and systems for providing a fiber layer thickness map based on optical coherence tomography images

Abstract

A system, arrangement, computer-accessible medium and process are provided for determining information associated with at least one portion of an anatomical structure. For example, an interference between at least one first radiation associated with a radiation directed to the anatomical structure and at least one second radiation associated with a radiation directed to a reference can be detected. Three-dimensional volumetric data can be generated for the at least one portion as a function of the interference. Further, the information can be determined which is at least one geometrical characteristic and/or at least one intensity characteristic of the portion based on the volumetric data.

Description

FIELD OF THE INVENTION

The present invention relates to processes, arrangements, computer-accessible medium and systems which can provide a fiber layer thickness map based on optical coherence tomography (“OCT”) images, and more particularly to such processes, systems, computer-accessible medium and arrangements that the boundaries and therefore the thickness of a layer in the sample can be automatically determined starting from OCT images.

BACKGROUND INFORMATION

Spectral-domain optical coherence tomography (“SD-OCT”) was recently established as a real-time technique for investigating the depth structure of biomedical tissue with the purpose of non-invasive optical diagnostics. A detailed description of SD-OCT techniques is described in Fercher et al. “Measurement of Intraocular Distances by Backscattering Spectral Interferometry”, Optics Communications, 117(1-2), 43 (1995) and Wojtkowski et al. “In vivo human retinal imaging by Fourier domain optical coherence tomography”, J. Biomed. Opt. 7(3), 457 (2002). Compared to the commercially available time-domain OCT systems, SD-OCT techniques provide for video-rate OCT scans, are relative fast, as shown in Nassif et al. “In vivo human retinal imaging by ultrahigh-speed spectral domain optical coherence tomography”, Opt. Lett. 29(5), 480 (2004), and provide a good sensitivity, as described in Leitgeb et al. “Performance of Fourier domain vs. time domain optical coherence tomography”, Opt. Express, 11(8), 889 (2003) and de Boer et al. “Improved signal-to-noise ratio in spectral-domain compared with time-domain optical coherence tomography”, Opt. Lett., 28(21), 2067 (2003). An exemplary arrangement which can be used for video-rate OCT scans has been described in International application number PCT/US03/02349 filed Jan. 24, 2003 and in Nassif et al. “In vivo human retinal imaging by ultrahigh-speed spectral domain optical coherence tomography”, Opt. Lett., 29(5), 480 (2004).

Similar technology, e.g., Optical Frequency Domain Imaging (“OFDI”), can use a rapidly tuned laser to measure the wavelength resolved interference as described in Chinn et al. “Optical coherence tomography using a frequency tunable optical source”, Opt. Lett. 22(5), 340 (1997), and Yun et al. “High-speed optical frequency-domain imaging”, Opt. Express 11(22), 2953 (2003) and International Application PCT/US04/029148 filed Sep. 8, 2004.

The depth profile in SD-OCT/OFDI can be obtained as the Fourier transform (“FFT”) of the spectral interference in a Michelson interferometer as described in Fercher et al. “Measurement of Intraocular Distances by Backscattering Spectral Interferometry”, Optics Communications, 117(1-2), 43 (1995) and Wojtkowski et al. “In vivo human retinal imaging by Fourier domain optical coherence tomography”, J. Biomed. Opt. 7(3), 457 (2002). The data processing steps to generate a good quality structural SD-OCT image have been described in Cense et al. “Ultrahigh-resolution high-speed retinal imaging using spectral-domain optical coherence tomography”, Opt. Express, 12(11), 2435 (2004), Yun et al. “High-speed optical frequency-domain imaging”, Opt. Express, 11(22), 2953 (2003), and Nassif et al. “In vivo high-resolution video-rate spectral-domain optical coherence tomography of the human retina and optic nerve”, Opt. Express, 12(3), 367 (2004). Various dispersion compensation techniques for OCT have been described in Marks et al. “Autofocus algorithm for dispersion correction in optical coherence tomography”, Appl. Opt., 42(16), 3038 (2003), Marks et al. “Digital algorithm for dispersion correction in optical coherence tomography for homogeneous and stratified media”, Appl. Opt., 42(2), 204 (2003), Wojtkowski et al. “Ultrahigh-resolution, high-speed, Fourier domain optical coherence tomography and methods for dispersion compensation”, Opt. Express, 12(11), 2404 (2004), and Fercher et al. “Numerical dispersion compensation for Partial Coherence Interferometry and Optical Coherence Tomography”, Opt. Express, 9(12), 610 (2001).

In ophthalmic applications, it has been suggested that OCT may be helpful for diagnosing glaucoma by measuring the thickness of the retinal nerve fiber layer (RNFL). In publications, the RNFL thickness has been evaluated with time-domain OCT commercial instruments for only a small number of circular scans, in general three, and not as a full map of the retina. A method to generate a large area thickness map of the RNFL is desirable. See e.g., Bourne et al. “Comparability of retinal nerve fiber layer thickness measurements of optical coherence tomography instruments” Invest. Opthalmol. Visual Sci., 46(4), 1280 (2005), Carpineto et al. “Reliability of nerve fiber layer thickness measurements using optical coherence tomography in normal and glaucomatous eyes” Opthalmology, 110(1), 190 (2003), Aydin et al. “Optical coherence tomography assessment of retinal nerve fiber layer thickness changes after glaucoma surgery”, Opthalmology, 110(8), 1506 (2003), and Guedes et al. “Optical coherence tomography measurement of macular and nerve fiber layer thickness in normal and glaucomatous human eyes”, Opthalmology, 110(1), 177 (2003).

Additional extensions of OCT techniques such as polarization-sensitive OCT (“PS-OCT”) can assist in identifying the properties of the RNFL including the layer's birefringence and boundaries as described in Cense et al. “In vivo birefringence and thickness measurements of the human retinal nerve fiber layer using polarization-sensitive optical coherence tomography”, J. Biomed. Opt., 9(1), 121 (2004), International Application PCT/US05/39374 filed Oct. 31, 2005, International Application PCT/US07/66017 filed Apr. 5, 2007 and International Application PCT/US06/15484 filed Apr. 24, 2006. It is believed that birefringence changes of the RNFL may preclude thickness changes and therefore, birefringence measurement can assist in early diagnosis of glaucoma.

Boundary detection has been studied since the early days of computer vision and image processing, and different approaches have been proposed. Segmentation procedures have also been applied to retinal imaging either for estimating the thickness of various retinal layers, as presented in Ishikawa et al. “Macular segmentation with optical coherence tomography”, Invest. Opthalmol. Visual Sci., 46(6), 2012 (2005) and Fernandez et al. “Automated detection of retinal layer structures on optical coherence tomography images”, Opt. Express, 13(25), 10200 (2005), or for evaluating the thickness of the retina, as presented in Koozekanani et al. “Retinal thickness measurements from optical coherence tomography using a Markov boundary model”, IEEE Trans. Medical Imag., 20(9), 900 (2001). Another segmentation technique based on a deformable spline (snake) algorithm has been described in details in Xu and Prince, “Snakes, shapes, and gradient vector flow” IEEE Trans. Image Process., 7(3), 359 (1998) and Kass et al. “Snakes—Active Contour Models”, Int. J. Comput. Vis., 1(4), 321 (1987). As the snake seeks to minimize its overall energy, its shape will converge on the image gradient contour. However, in general, the snake may not be allowed to travel extensively, and proper initialization may be needed. The snake parameters (elasticity, rigidity, viscosity, and external force weight) can be set to allow the snake to follow the boundary for a large number of retinal topographies. Deformable spline procedures are widely used in medical imaging.

A RNFL thickness map is a quantitative assessment and provides evaluation of large retinal areas as compared to a limited number of circular or radial scans measured with the current commercial instruments. The RNFL thickness maps can potentially be used for a thorough evaluation of the RNFL thickness in longitudinal studies of glaucoma progression. These procedures use large area RNFL thickness maps, which may allow for more accurate correlations of RNFL thinning with visual field defects as opposed to individual circular or radial scans that should be measured at precisely the same retinal location, which is very difficult and that give less information. Therefore, a methodology that allows a determination of RNFL thickness maps based on noise suppression and edge detection may be desirable. Also an intuitive representation of OCT data may be desirable for diagnostic purposes by correlating the quantitative RNFL thickness map with an ultra-high resolution OCT movie, therefore providing a comprehensive picture to clinicians.

Accordingly, there is a need to overcome the deficiencies as described herein above.

OBJECTS AND SUMMARY OF EXEMPLARY EMBODIMENTS

To address and/or overcome the above-described problems and/or deficiencies, exemplary embodiments of processes, systems, computer-accessible medium and arrangements that the boundaries and therefore the thickness of a layer in the sample can be automatically determined starting from OCT images. For example, exemplary processes, systems, computer-accessible medium and arrangements may be provided for determining the thickness of retinal layers including but not limited to the RNFL.

According to one exemplary embodiment of the present invention, it is possible to implement the procedures, systems and arrangements described in U.S. Pat. No. 6,980,299 and International Application No. PCT/US04/023585 filed Jul. 23, 2004

The exemplary embodiments of the procedures, systems, computer-accessible medium and arrangements according to the present invention can be used to identify the boundaries of the retinal layers, such as but not limited to the anterior and posterior RNFL boundaries. In further exemplary embodiments, the retinal layers can by defined and be differentiated based on various characteristics, including but not limited to the magnitude and/or standard deviation of intensity reflectance, polarization properties, texture, and/or Doppler properties.

In addition, the exemplary embodiments of the procedures, systems, computer-accessible medium and arrangements according to the present invention can be used to determine the retinal surface topography and the topography of the optic nerve head (“ONH”). High-resolution characterization of the ONH topography can be interesting for a quantitative assessment of glaucoma. Further, another exemplary embodiment of the procedures, systems and arrangements according to the present invention can be used to determine the boundaries of the retinal pigment epithelium (“RPE”). The shape of the RPE may be interesting in the analysis of retinal drusen. Yet further exemplary embodiments of the procedures, systems, computer-accessible medium and arrangements according to the present invention are capable of quantifying the retinal nerve fiber tissue by measuring the RNFL thickness and the thickness distribution across large areas of the retina.

Thus, according to the exemplary embodiments of the present invention, it is possible to:

• • a. determine layer boundaries, including but not limited to the anterior and posterior boundaries of the RNFL;
  • b. determine the properties of the RPE and the optic disc as the edge of the RPE;
  • c. determine the RNFL thickness and thickness distribution over large areas of the retina;
  • d. determine the geometry, the shape and volume of anatomical structures including but not limited to the ONH cup;
  • e. use model-based extraction of retinal properties starting from know structural characteristics.

Still another exemplary embodiment of the procedures, systems, computer-accessible medium and arrangements according to the present invention are capable of facilitating clinical interpretation of the OCT data. A display modality, as an exemplary embodiment, can combine the thickness map and a reflectivity map (e.g., a fundus-type image), together with the cross-sectional images of the retina (e.g., OCT movie).

In yet another exemplary embodiment of the procedures, systems, computer-accessible medium and arrangements according to the present invention, different images can be combined with their difference and/or ratio to illustrate features not evident from either of the two images. For example, the two images can be 3D volumes, cross-sectional OCT frames and or thickness maps. Such exemplary images may be obtained from measurements taken at different patient visits and the difference between them could indicate changes as a result of disease progression.

According to still further exemplary embodiment of the present invention, the measurement may be performed on the same eye using light from different spectral bands. The scattering/reflectivity/absorption properties of the ocular tissue can depend on the wavelength of light, and therefore, measurements performed within different wavelength bands could potentially reveal different structural and morphological information.

In yet another exemplary embodiment of the present invention, these exemplary images may be different due to, e.g., external stimuli or factors including but not limited to light, medication, or blood pressure, and therefore, the difference or ratio image could reveal functional properties of the ocular tissue.

Thus, according to one exemplary embodiment of the present invention, a system, arrangement, computer-accessible medium and process may be provided for determining information associated with at least one portion of an anatomical structure. For example, an interference between at least one first radiation associated with a radiation directed to the anatomical structure and at least one second radiation associated with a radiation directed to a reference can be detected. Three-dimensional volumetric data can be generated for the at least one portion as a function of the interference. Further, the information can be determined which is at least one geometrical characteristic and/or at least one intensity characteristic of the portion based on the volumetric data.

For example, the first radiation can be generated by a low coherence source, and the interference may be detected simultaneously for separate wavelengths that are different from one another. The first radiation can also be generated by an automatically wavelength-tuned light source. The anatomical structure can be an ocular structure. The geometrical characteristic can include at least one continuous boundary. The generation of the continuous boundary can be based on:

• • first data associated with a scattered intensity and/or a polarization state of the interference,
  • second data associated with a distribution which is a spatial distribution and/or a temporal distribution of intensity variations of the interference, and/or
  • third data associated with a motion of scattering objects within the anatomical structure.

Further, the boundary can define a topological structure, and the information may include a geometry, a curvature, a volume and/or a thickness of the topological structure. It is also possible to generate at least one visualization associated with the information. The visualization can be at least one image. In addition, it is possible to determine at least one change of the information as a function of at least one condition.

According to yet another exemplary embodiment of the present invention, it is possible to filter the three-dimensional volumetric data based on a priori knowledge associated with the anatomical structure, and the information may be determined as a function of the filtered volumetric data. The priori knowledge can be based on at least one characteristic of a system performing such functions. The priori knowledge can also be based on at least one characteristic of a known progression of at least one abnormality associated with the anatomical structure.

In still another exemplary embodiment of the present invention, the first radiation can comprise a first radiation signal provided at a first wavelength range and a second radiation signal provided at a second wavelength range which is different from the first range. The three-dimensional volumetric data may be generated as a function of the first and second radiation signals. The first radiation can further comprise a third radiation signal provided at a third wavelength range which is different from the first and second ranges. Thus, the three-dimensional volumetric data may be generated as a function of the first, second and third radiation signals, and the information can be a color volume of the portion of the anatomical structure.

These and other objects, features and advantages of the present invention will become apparent upon reading the following detailed description of embodiments of the invention, when taken in conjunction with the appended claims.

BRIEF DESCRIPTION OF THE DRAWINGS

Further objects, features and advantages of the invention will become apparent from the following detailed description taken in conjunction with the accompanying figures showing illustrative embodiments of the invention, in which:

FIGS. 1A(a) through 1A(l) are exemplary illustrations of images takes during an implementation of an exemplary embodiment of a process for locating, e.g., RNFL boundaries and thickness according to the present invention;

FIG. 1B is a top level flow diagram of the exemplary embodiment of the process according to the present invention;

FIG. 1C is a detailed flow diagram of a first step of the exemplary process shown in FIG. 1B;

FIG. 1D is a detailed flow diagram of a second step of the exemplary process shown in FIG. 1B;

FIGS. 2A and 2B are selected cross-sectional frames of moving images of the OCT scans indicating the anterior and posterior boundary of the RNFL obtained using the exemplary procedures, systems and arrangements according to the present invention;

FIGS. 3B and 3A are exemplary integrated reflectance images obtained using the exemplary procedures, systems and arrangements according to the present invention as compared to the resultant images obtained using other technologies on the same eye;

FIG. 4 is an exemplary RNFL thickness map obtained using the exemplary procedures, systems and arrangements according to the present invention;

FIGS. 5A(top) and 5B(top) are combined exemplary representations of an integrated reflectance map obtained using the exemplary procedures, systems and arrangements according to the present invention;

FIGS. 5A(bottom) and 5B(bottom) are combined exemplary representations of a RNFL thickness map using the exemplary procedures, systems and arrangements according to the present invention;

FIGS. 5C and 5D are combined exemplary representations of retinal cross-sectional images obtained using exemplary procedures, systems and arrangements according to the present invention;

FIGS. 6A and 6B are images of two exemplary RNFL thickness maps;

FIG. 6C is an exemplary image map with is indicative of the difference between the exemplary images of FIGS. 6A and 6B; and

FIG. 7 is an exemplary embodiment of the system/arrangement according to the exemplary embodiment of the present invention which is configured to perform exemplary processes and/or procedures according to the present invention.

Throughout the figures, the same reference numerals and characters, unless otherwise stated, are used to denote like features, elements, components or portions of the illustrated embodiments. Moreover, while the subject invention will now be described in detail with reference to the figures, it is done so in connection with the illustrative embodiments. It is intended that changes and modifications can be made to the described embodiments without departing from the true scope and spirit of the subject invention as defined by the appended claims.

DETAILED DESCRIPTION OF EXEMPLARY EMBODIMENTS

The exemplary embodiments of procedures, systems and arrangements according to the present invention which is configured to process data for determining an RNFL thickness can involve, e.g., certain steps of edge detection. In one such exemplary embodiment, the exemplary process can be performed frame by frame in 2D by identifying the edges corresponding to the anterior and posterior boundaries of the RNFL 1000 as shown in FIG. 1A(b). According to another exemplary embodiment, the analysis can be performed in 3D thereby extending the exemplary embodiment described herein above from being a 2D analysis to a 3D analysis.

Particularly, FIGS. 1A(a) through 1A(l) are exemplary illustrations of images takes during an implementation of an exemplary embodiment of a process for locating, e.g., RNFL boundaries and thickness according to the present invention. FIG. 1B is a top level flow diagram of the exemplary embodiment of the process according to the present invention. FIG. 1C is a detailed flow diagram of a first step of the exemplary process shown in FIG. 1B, and FIG. 1D is a detailed flow diagram of a second step of the exemplary process shown in FIG. 1B.

The first step (100) of the exemplary process of FIG. 1B is provided to identify the anterior boundary (“AB”) 1010 of the RNFL 1000 shown in FIG. 1A(b). Certain preliminary steps can be performed to determine an initial guess result for AB 1010. The image can be blurred using a Gaussian kernel (step 100-10 of FIG. 1C) for smoothing out the edges present in the image while suppressing spurious artifacts due to imaging noise. The standard deviation of the kernel can be set statistically with respect to the depth size of the image. The edge image is calculated as the magnitude of the image gradient, and rescaled between 0 and 1 by subtracting its minimum value and normalizing to its maximum value. The edge image is then converted to a binary image by keeping all edges above a threshold value. (Step 100-20 of FIG. 1C). This threshold can be determined such that AB 1010 remains a continuous line in the edge image.

Certain areas in the OCT scan, e.g., around the ONH and the fovea, may contain weak edges that should still to be identified, and such procedure can indicate how low the threshold should be set. Certain false edges are, however, preserved this way due to the noise in the image. They could be eliminated or reduced by removing any object in the binary image that has an area smaller than a certain percentage of the total image size determined based on analyzing a large number of images. The exemplary purpose is to preserve preferably the continuous lines across the image, and therefore this value could be set based on the size of the image. The exemplary result is shown in the image of FIG. 1A(a).

The initial guess for AB 1010 can then be determined as the first unity pixel from the top in the binary edge image along each column (step 100-30 of FIG. 1C). To avoid holes in the identified AB 1010, the columns that contain no edge may be removed and then AB 1010 can be linearly interpolated over the removed A-lines. A median filter with a moving window may be applied to smooth out the AB 1010. (Step 100-40 of FIG. 1C). The size of the moving window can be set statistically with respect to the lateral size of the image.

This exemplary initial guess of AB 1010 may be used as initialization for a multiresolution deformable spline algorithm/procedure. The external force field for the snake algorithm/procedure may be obtained as the gradient of the edge image that was generated as described above for a Gaussian kernel (step 100-60 of FIG. 1C) with a standard deviation radius set statistically with respect to the size of the image. The purpose of the Gaussian blur, as described earlier, is to make sure the initial guess for AB 1010 is within the capture range of the true boundary at AB 1010. This exemplary procedure also determines the resolution in finding AB 1010. Further the multiresolution deformable spline algorithm/procedure can be applied to the result (step 100-70 of FIG. 1C). The exemplary procedure can then be repeated (step 100-80 of FIG. 1C) with a smaller value of the standard deviation of the kernel (see FIG. 1A(b)), therefore a better resolution, using as initialization the value of AB 1010 obtained from the previous run of the algorithm with a coarse resolution.

The anterior boundary of the RNFL 1000 can be used to create and display the 3D topography of the retinal surface and of the ONH. (Step 100-90 of FIG. 1C). The knowledge of the topography of the retinal surface can be important for determining the geometry, the shape and volume of retinal structures including but not limited to the ONH cup. The geometrical properties of the ONH cup may be used for quantitative characterization of glaucoma.

The second step in determining the RNFL thickness is to identify the posterior boundary (“PB”) 1140 of the nerve fiber layer (step 110 of FIG. 2B). As the transition between the RNFL 1000 and the ganglion cell layer may not be as sharp and uniform as between the vitreous humor and the retina, another exemplary procedure according to one exemplary embodiment of the present invention can be used for identifying the PB 1140 (FIG. 1A(l)). There may be a shadow cast by the blood vessels 1020 from the RNFL 1000 that may generate “holes” 1040 in the PB 1140. Further, there may be little or no RNFL 1000 in the ONH area (e.g., the nerve fibers may be provided along the optic nerve, perpendicular to the retina, and therefore parallel to the OCT beam). If the nerve fibers are perpendicular to the incident laser beam, they can be detected as a layer. However, if these nerve fibers are positioned parallel to the OCT beam (as may be in the optic nerve), it may be difficult to detect them, as there is no “horizontal” boundary (e.g., perpendicular to the laser beam) to reflect the light.

Certain exemplary preliminary steps can be taken before the actual estimation of the PB 1140. As an initial matter, everything above the AB 1010 can be removed (step 110-5 of FIG. 1D). The image may be realigned to AB 1010 based on the assumption that the anterior and posterior boundaries are relatively parallel and the procedure in determining PB 1140 may be more stable for primarily horizontal edges. A certain depth can be maintained along each A-line. This exemplary depth may be selected to include certain relevant part of the depth profiles. Most or all of the images shown in FIGS. 1A(c) to 1A(k) can have AB 1010 as the top edge, and may preferably represent the steps in determining the PB 1140.

Further, the image can be processed to generate the smoothed field f (FIG. 1A(c)) and the edge field s (FIG. 1A(d)) by using an algorithm for joint anisotropic smoothing and edge-preservation. (Step 110-10 of FIG. 1D). The edge field s is the rescaled (between 0 and 1) magnitude of the gradient of f, as described above. The exemplary procedure can be based on a conjugate gradient based iterative minimization of a cost functional described in Barrett et al. “Templates for the Solution of Linear Systems: Building Blocks for Iterative Methods”, 2nd ed. 1994, Philadelphia, Pa.: SIAM, which can balance a data fidelity term against prior models for image smoothness and edge density as described in Chan et al. “Anisotropic edge-preserving smoothing in carotid B-mode ultrasound for improved segmentation and intima-media thickness (IMT) measurement” in IEEE Computers in Cardiology 2000, Cambridge, Mass., USA, and Chan et al. “A variational energy approach for estimating vascular structure and deformation from B-mode ultrasound imagery” in IEEE International Conference on Image Processing. 2000. Vancouver, BC, Canada. The cost functional is provided by:

$\begin{array}{cc}E\left(f,s\right)=\int \left(\beta {f-g}_1+{\alpha \left(1-s\right)}^2{\nabla f}_1+\frac{\rho }{2}{\nabla s}_2^2+\frac{1}{\rho }{s}^2\right)dA& \left(1\right)\end{array}$ where the notation ∥.∥_k represents an l_k norm (k=1, 2), and the integration is done over the entire image.

The first term can represent the data fidelity and controls the degree to which the smoothed field f resembles the original image g. The second term, representing the smoothness constraint, may penalize large gradients in f except where edges exist (s 1), generating the greatest anisotropic smoothing far away from the edges. The last two terms, representing the edge penalty, can control the edge width and prevent the minimization process from placing edges everywhere in the edge field s. The real positive scalars α, β, and ρ can adjust the relative weighting between these competing terms. The solution of Eq. (1) may be obtained by iterative minimization of the cost functional until convergence to a predefined tolerance level is achieved or an exemplary maximum number of iterations can be exceeded. The subsequent steps in the image processing may be based on f and s, and preferably not the original image.

In a further exemplary embodiment of the present invention, the original image g in Eq. (1) can be replaced by a model image based on a priori knowledge of the retinal structure. In a normal retina, the structure, the properties, and the number of the layers are known, and a model based extraction of the layers' boundaries can be used. Deviations from the model can indicate pathologies and could help in diagnosing retinal diseases.

An identification of blood vessels 1020 position in the RNFL 1000 can also be beneficial prior to the estimation of the PB 1140. This can be done based on the analysis of the RPE 1030. Scattering and absorption of the OCT beam due to the blood can significantly reduce the ability of the OCT beam to probe behind the blood vessels 1020, and the structural image (FIG. 1A(b)) appears to have a “shadow” underneath the blood vessels 1020. This can generate “holes” 1040 in the PB 1140 as well as in the RPE 1030. The RPE 1030 can be identified in the image, and the index of the A-lines corresponding to these “holes” 1040 can be estimated. These indices, that may be declared as invalid, can later be used in the analysis of the PB 1140.

The identification of the RPE 1030 may be based on both the magnitude of the smoothed field f and its gradient, e.g., the edge field s. An intensity mask (FIG. 1A(e)) may be generated from the smoothed field f based on the statistical properties of f, mean and standard deviation, using mean(f)−std(f) as threshold. (Step 110-15 of FIG. 1D). A binary image may also be created by thresholding the edge field s. (Step 110-17 of FIG. 1D). The threshold value can be selected as described above to preserve the weaker edges. Small patches may be removed from the binary edge image to clear out spurious points. The lowest (deepest) pixel with value one along each A-line can be selected from the two binary images as the posterior boundary of RPE 1030. (Step 110-20 of FIG. 1D). This boundary is then smoothed out with a moving window median filter. A band 1070 (FIG. 1A(f)) with a predefined thickness above the posterior RPE boundary 1030 is then selected from the smoothed field f and is averaged along the A-lines to generate a mean value of the RPE reflectance 1080 along each A-line (see dots in FIG. 1A(f)). (Step 110-25 of FIG. 1D). The mean RPE reflectance 1080 is then filtered out 1090 using a Savitzky-Golay FIR smoothing filter (black line in FIG. 1A(f)) that fits the data with a third order polynomial in a moving window. The index of an A-line is determined as invalid if the mean RPE value 1080 drops on that A-line by more than a certain predefined value as compared to the filtered mean RPE 1090. (Step 110-30 of FIG. 1D). As mentioned above, these invalid indices can correspond to the “holes” 1040 in the RPE 1030 generated by the shadow of the blood vessels 1020. Such indices may also correspond to the ONH area where there is no RPE 1030. The invalid indices are extended by a number of 10 A-lines on both sides of the shadows, as identified above, just to make sure that the vertical edges corresponding to the boundary of the shadows are removed from the image. Generally, the blood vessels 1020 have a larger diameter than the holes 1040 identified in the RPE 1030.

In yet another exemplary embodiment of the present invention, a map of the blood vessels network and the boundaries of the optic disc can be determined from the entire 3D OCT scan rather than frame by frame. After identifying the AB 1010, it is possible to remove from the 3D OCT scan a band below the AB 1010 that may include the RNFL 1000 and then integrate the depth profiles generating a RPE map. Integrating preferably only the layers below the RNFL 1000 can increase the contrast of the RPE map since the RPE 1030 is likely the strongest reflecting layer below the RNFL 1000. Appropriate thresholding and segmentation of the RPE map may provide the invalid A-lines (indices) described above, as well as the boundaries of the optic disc that can be used subsequently for identifying the PB 1140.

The RPE area 1060 can be removed from the smoothed field f, the intensity mask, and the binary edge image, and the rest of the processing is focused on the posterior boundary 1140 of the RNFL 1000. (Step 110-35 of FIG. 1D). The intensity mask 1050 may be applied to the edge field s in order to remove the edges that are outside the interest area. (Step 110-40 of FIG. 1D). To avoid broken lines, the binary edge image may be dilated and then eroded (FIG. 1A(g)). A morphological thinning operation is then performed on the binary edge image. (Step 110-45 of FIG. 1D). Vertical and negative edges are removed since predominantly horizontal edges with the correct slope from the RNFL 1000 to the ganglion cell layer (FIG. 1A(h)) are being looked for. (Step 110-50 of FIG. 1D).

An initial guess of the PB 1140 can be estimated as the first pixel of value one from the top along each A-line (see white dots 1100 in FIG. 1A(i)). (Step 110-55 of FIG. 1D). For the A-lines that have no pixel of value 1 in the binary edge image, the PB 1140 can be set to coincide with AB 1010. This exemplary situation may correspond to the areas around the ONH and fovea. The columns with invalid indices may be removed and the PB 1140 is linearly interpolated over the invalid regions. (Step 110-60 of FIG. 1D). To confirm that the PB 1140 is relatively smooth, the smoothing procedure described above for the RPE analysis employing a Savitzky-Golay FIR smoothing filter can be used, as well with a moving window (see black line 1110 in FIG. 1A(i)). This exemplary step can be used to remove points that are too far from the smoothed version of PB 1140.

At this point, the deformable spline algorithm/procedure can be applied. The intensity mask 1050 is applied to the original edge field s, and the edge field is then blurred with a Gaussian kernel. The external forces are calculated as gradient of the rescaled edge field, and they are set to zero for the A-lines with invalid indices. (Step 110-65 of FIG. 1D). The A-lines with invalid indices are removed from the result of the snake algorithm (1120 in FIG. 1A(j)) and PB 1140 is linearly interpolated over the invalid regions. (Steps 110-70 and 110-75 of FIG. 1D). A final median filter with a moving window can be applied to the calculated PB 1130 (FIG. 1A(k)). (Step 110-75 of FIG. 1D). Since the image has been realigned to the anterior boundary, the result obtained can preferably be the RNFL thickness. With respect to the original image, it is possible to add this result to the AB 1010 values to obtain the true or accurate PB 1140 (FIG. 1A(l)). (Step 110-80 of FIG. 1D).

The exemplary results of the exemplary procedure according to the present invention described above are shown in FIG. 1A(l) by displaying the identified AB 1010 and PB 1140 on the corresponding structural image. The exemplary parameters in the process, system and arrangement according to the exemplary embodiments of the present invention, such as threshold values, snake parameters for anterior and posterior boundaries, and RPE thickness, can be established based on a large number of OCT scans in different areas of the retina and for different subjects to account for a statistically significant variability in the boundaries' characteristics. The snake parameters can be set differently for AB 1010 and PB 1140 given the different properties of the two boundaries. The exemplary data sets described herein can be processed with fixed settings for AB 1010 and PB 1140.

According to another exemplary embodiment of the present invention, as shown in FIGS. 2A and 2B, can provide examples of RNFL boundaries AB 2000 and 2020 and PB 2010 and 2030 as determined by the exemplary embodiment of an automated procedure according to the present invention. For example, a video-rate OCT movie can be difficult to follow and interpret. It is not always clear what is occurring with the blood vessels moving laterally in the image and with the continuous and sometimes sudden change in their apparent diameter. If the orientation of the blood vessel changes from frame to frame, it may appear in the OCT-movie that the diameter of the blood vessel changes. There bay be certain situation that in the OCT-movie, the vessel can be provided parallel to the frame, and it may “appear” very thick, and then in the next frame it can be visualized as being very thin, since it changed its orientation with respect to the frame. Additional information may be useful for determining the correct interpretation of OCT-movies.

Previously, a visualization has been demonstrated where a fundus-type image was shown as a still picture simultaneously with the OCT movie—see Jiao et al. “Simultaneous acquisition of sectional and fundus ophthalmic images with spectral-domain optical coherence tomography”, Opt. Express, 13(2) 444 (2005). A line across this picture indicated the position of the OCT scan for orientation along the retinal surface. This picture was obtained by integrating the depth profiles (the reflectance) and was displayed on a logarithmic scale. This operation creates enough contrast to differentiate between the A-lines that correspond to blood vessels' location and those that do not intersect blood vessels. The scattering and absorption on blood reduce the total reflectance in the area corresponding to blood vessels and the vessels appear darker than the surroundings.

According to the exemplary embodiment of the present invention, a smoother image can be obtained by, e.g., integrating the logarithmic depth profile and displaying it in linear scale as shown in the exemplary images on the right sides of FIGS. 3A and 3B. The integrated reflectance image can be compared in FIGS. 3A and 3B to images of the same area in the same eye obtained with different procedures, e.g., fundus imaging and fluoresce in angiography, respectively.

As compared to a fundus image of the same eye (as shown in the left side of FIG. 3A), the integrated reflectance image illustrates the same structure of the blood vessels 3000 with a very good quality, approaching that of a fundus photo. FIG. 3B shows an angiogram (side left) and the integrated reflectance image (right side) for the same area around the fovea 3030. The images of FIGS. 3A and 3B demonstrate that the integrated reflectance map can be used as a reliable representation of the retinal vasculature 3000 and 3040, ONH 3010, and fovea 3020 and 3030. The integrated reflectance image can be obtained directly from the OCT data, and may not need to utilize additional imaging procedures. The ability to provide an accurate representation of the retina it is also beneficial to clinicians.

The experimental measurements described herein above were performed on the right eye of a healthy volunteer. According to another exemplary embodiment of the present invention as shown in FIG. 4, a map of the RNFL thickness can be obtained using the exemplary procedure described herein. For example, the RNFL thickness map can be smoothed out with a median filter. The darkest areas in FIG. 4 represent the absence of the RNFL, corresponding to the fovea 4000 and ONH 4010. The lighter area corresponds to thinner areas of the RNFL, while other darker areas represent thicker RNFL areas. Such RNFL map may be consistent with known normal retinal anatomy, as the RNFL thickness may have greater superior and inferior to the ONH. This exemplary image map can provide a quantitative assessment of the RNFL thickness and a comprehensive evaluation of large retinal areas as opposed to a limited number of circular or radial scans measured with the current commercial instruments.

In another exemplary embodiment of the present invention FIGS. 5A-5D illustrate the combined retinal information analyzed herein. For example, FIGS. 5A(top) and 5B(top) show the exemplary integrated reflectance as a map of the retina. FIGS. 5A(bottom) and 5B(bottom) show the exemplary RNFL thickness map. FIGS. 5C and 5D shown frames of a movie of a video-rate OCT scan indicating the boundaries of the RNFL, e.g., AB 5040 and 5090 (FIGS. 5C and 5D, respectively), and PB 5050 and 5100 (FIGS. 5C and 5D, respectively). Using this exemplary display modality, it is possible to better follow in the movie the structure of the blood vessels pattern 5020 and 5080 (FIGS. 5A and 5B, respectively). The position of each depth scan, indicated by the horizontal red line 5010 and 5060 (FIGS. 5A and 5B, respectively) across the maps, can be related to retinal morphology, i.e. the ONH 5030 (FIG. 5A) and the fovea 5000 and 5070 (FIGS. 5A and 5B, respectively).

The position of the blood vessels across the cross-sectional images, indicated by their “shadow”, can be correlated with the intersection of the horizontal line with the vasculature evident in the integrated reflectance map. The integrated reflectance map may also illustrate the orientation of the blood vessels with respect to the cross-sectional scans, thus allowing for a clear interpretation of the continuous and sometimes sudden change in the apparent diameter of the blood vessels. The association of the integrated reflectance map and of the RNFL thickness map with the OCT movie can provide the clinicians a more intuitive way of interpreting the OCT data for diagnosing retinal diseases such as glaucoma. FIGS. 5A and 5C show illustrations of a large area OCT scan including the ONH 5030 and the fovea 5000. FIGS. 5B and 5D show an exemplary OCT scan centered on the fovea 5070, which also illustrate the vasculature around the fovea and the retinal depth structure with a greater detail as compared to FIGS. 5A and 5C.

The dark band on the center left side of the RNFL thickness map shown in FIG. 5B(bottom) can correspond to the temporal raphe, a structure located temporal to the macula. Since it may be difficult to distinguish individual fibers, it is also difficult to see the structure and the direction of the retinal nerve fibers in the thickness map. However, the RNFL thickness is small in the raphe area since there are a limited number of fibers. Moving away from the raphe, additional fibers comprise the RNFL and the thickness likely increases. The exemplary RNFL thickness map obtained according to the exemplary embodiments of the present invention may be consistent with the RNFL distribution pattern described in Vrabec “Temporal Raphe of Human Retina”, Am. J. Opthalmol., 62(5), 926 (1966) that was confirmed later on by opthalmoscopy as described in Sakai et al. “Temporal Raphe of the Retinal Nerve-Fiber Layer Revealed by Medullated Fibers”, Jpn. J. Opthalmol., 31(4), 655 (1987).

According to yet a further exemplary embodiment of the present invention, two exemplary RNFL thickness maps 6000, 6010 corresponding to the same scan area on the same eye can be obtained as shown in FIGS. 6A and 6B, respectively, and the difference between them is shown in an image 6020 of FIG. 6C. These exemplary RNFL thickness maps 6000, 6010 can be obtained based on the exemplary measurements taken at different patient visits, and the difference image 6020 between them may indicate changes as a result of disease progression.

In still another exemplary embodiment of the present invention, the measurement can be performed on the same eye using light from different spectral bands. The scattering/reflectivity/absorption properties of the ocular tissue can depend on the wavelength of light, and therefore, measurements performed with different wavelength bands may potentially reveal different structural and morphological information. The exemplary images 6000, 6010 shown in FIGS. 6A and 6B can be the result of such measurements, and the exemplary image 6020 of FIG. 6C may be the difference or the ratio of the images 6000, 6010 of FIGS. 6A and 6B illustrating exemplary features not evident in either FIG. 6A or 6B. In yet another exemplary embodiment, the exemplary RNFL thickness maps 6000, 6010 shown in FIGS. 6A and 6B can be different due to external stimuli or factors such as light, medication, or blood pressure, and therefore, the exemplary difference or ratio image 6020 of FIG. 6C can reveal functional properties of the ocular tissue.

In still another exemplary embodiment of the present invention, the exemplary 3D OCT scans can be acquired for multiple (e.g., three) different wavelength bands and the structural information obtained in each wavelength band can be mapped to a color system including but not limited to the RGB system. A color volume representation of the OCT data may provide structural and morphological information not otherwise evident.

The above-described exemplary embodiments of the processes and procedures according to the present invention can be performed by processing arrangements described in a number of patent applications referenced herein. For example, one exemplary embodiment of the system/arrangement according to the exemplary embodiment of the present invention which is configured to perform such exemplary processes and/or procedures is shown in FIG. 7. In particular, an exemplary arrangement 7020 can be provided, which may include an interferometric arrangement 7030, a processing arrangement (e.g., a microprocessor, a computer, etc.) 7040, and a storage arrangement/computer accessible medium (e.g., hard disk, CD-ROM, RAM, ROM, etc.) 7050.

In the exemplary operation of the system/arrangement according to one embodiment of the present invention shown in FIG. 7, the interferometric arrangement 7020 can be configured to receive radiation from an anatomical structure 7000 and a radiation from a reference 7010, and detect an interference there between. The processing arrangement 7040 can access the storage arrangement/computer accessible medium 7050 to obtain instructions and/or software provided or stored thereon. As an alternative, the processing arrangement 7040 can have such instructions/software previously provided therein. These instructions/software can be executed by the processing arrangement 7040 so that it can be configured to receive the interference information associated with the determined interference, and generate three-dimensional volumetric data for at least one portion of the anatomical structure as a function of the interference. Then, such configured processing arrangement 7040 can determine and provide the information 7060 which is at least one geometrical characteristic and/or at least one intensity characteristic of such portion of the anatomical structure based on the volumetric data.

The foregoing merely illustrates the principles of the invention. Various modifications and alterations to the described embodiments will be apparent to those skilled in the art in view of the teachings herein. Indeed, the arrangements, systems and methods according to the exemplary embodiments of the present invention can be used with any OCT system, OFDI system, SD-OCT system or other imaging systems, and for example with those described in International Patent Application PCT/US2004/029148, filed Sep. 8, 2004, U.S. patent application Ser. No. 11/266,779, filed Nov. 2, 2005, and U.S. patent application Ser. No. 10/501,276, filed Jul. 9, 2004, the disclosures of which are incorporated by reference herein in their entireties. It will thus be appreciated that those skilled in the art will be able to devise numerous systems, arrangements and methods which, although not explicitly shown or described herein, embody the principles of the invention and are thus within the spirit and scope of the present invention. In addition, to the extent that the prior art knowledge has not been explicitly incorporated by reference herein above, it is explicitly being incorporated herein in its entirety. All publications referenced herein above are incorporated herein by reference in their entireties.

Claims

1. A system for determining information associated with at least one portion of an anatomical structure, comprising: at least one arrangement configured to:a. detect an interference between at least one first radiation associated with a radiation directed to the anatomical structure and at least one second radiation associated with a radiation directed to a reference,b. generate three-dimensional volumetric data for the at least one portion as a function of the interference, andc. determine the information based on the volumetric data and at least one of (i) a spatial distribution or (ii) a temporal distribution of an intensity of the interference.

2. The system according to claim 1, wherein the at least one first radiation is generated by a low coherence source.

3. The system according to claim 2, wherein the interference is detected simultaneously for separate wavelengths that are different from one another.

4. The system according to claim 1, wherein the at least one first radiation is generated by an automatically wavelength-tuned light source.

5. The system according to claim 1, wherein the anatomical structure is an ocular structure.

6. The system according to claim 1, wherein the information comprises at least one geometrical characteristic which includes at least one continuous boundary.

7. The system according to claim 6, wherein the at least one arrangement is further configured to generate the at least one continuous boundary based on at least one of: first data associated with a distribution which is at least one of the spatial distribution or the temporal distribution of intensity variations of the interference, orsecond data associated with a motion of scattering objects within the anatomical structure.

8. The system according to claim 6, wherein the at least one boundary is overlaid over an image of the at least one portion to generate a topological structure.

9. The system according to claim 8, wherein the at least one arrangement is further configured to generate at least one visualization of the topological structure associated with the information.

10. The system according to claim 9, wherein the at least one visualization is at least one image.

11. The system according to claim 8, wherein the at least one arrangement is further configured to determine at least one change of the information as a function of at least one condition.

12. The system according to claim 1, wherein the at least one arrangement is further configured to filter the three-dimensional volumetric data based on a priori knowledge associated with the anatomical structure, and wherein the information is determined as a function of the filtered volumetric data.

13. The system according to claim 12, wherein the priori knowledge is based on at least one characteristic of the system anatomical structure.

14. The system according to claim 12, wherein the priori knowledge is based on at least one characteristic of a known progression of at least one abnormality associated with the anatomical structure.

15. The system according to claim 1, wherein the at least first radiation comprises a first radiation signal provided at a first wavelength range and a second radiation signal provided at a second wavelength range which is different from the first range, and wherein the three-dimensional volumetric data is generated as a function of the first and second radiation signals.

16. The system according to claim 15, wherein the at least one first radiation further comprises a third radiation signal provided at a third wavelength range which is different from the first and second ranges, and wherein the three-dimensional volumetric data is generated as a function of the first, second and third radiation signals, and wherein the information is a color volume of the at least one portion of the anatomical structure.

17. A process for determining information associated with at least one portion of an anatomical structure, comprising: detecting an interference between at least one first radiation associated with a radiation directed to the anatomical structure and at least one second radiation associated with a radiation directed to a reference;generating three-dimensional volumetric data for the at least one portion as a function of the interference; anddetermining the information based on the volumetric data and at least one of (i) a spatial distribution or (ii) a temporal distribution of an intensity of the interference.

18. A computer accessible medium for determining information associated with at least one portion of an anatomical structure, and providing thereon a software program, which, when executed by a processing arrangement, is operable to perform the procedures comprising: detecting an interference between at least one first radiation associated with a radiation directed to the anatomical structure and at least one second radiation associated with a radiation directed to a reference;generating three-dimensional volumetric data for the at least one portion as a function of the interference; anddetermining the information based on the volumetric data and at least one of (i) a spatial distribution or (ii) a temporal distribution of an intensity of the interference.

19. The computer accessible medium according to claim 18, wherein the processing arrangement, when the software is executed thereby, is configured to perform further procedures comprising: separating different wavelengths of the interference via a dispersive arrangement; andsimultaneously detecting the interference for the different wavelengths using a plurality of detectors.

20. The system according to claim 1, wherein the at least one arrangement is further configured to: d. separate different wavelengths of the interference via a dispersive arrangement; ande. simultaneously detect the interference for the different wavelengths using a plurality of detectors.