|Publication number||USRE42497 E1|
|Application number||US 12/205,248|
|Publication date||Jun 28, 2011|
|Filing date||Sep 5, 2008|
|Priority date||May 6, 2003|
|Also published as||US7102758, US20040223162, WO2004102109A2, WO2004102109A3|
|Publication number||12205248, 205248, US RE42497 E1, US RE42497E1, US-E1-RE42497, USRE42497 E1, USRE42497E1|
|Original Assignee||Duke University|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (70), Non-Patent Citations (37), Referenced by (6), Classifications (5), Legal Events (2)|
|External Links: USPTO, USPTO Assignment, Espacenet|
1. Field of the Invention
The present invention relates to an apparatus and method for obtaining depth-resolved spectra for the purpose of determining structure by measuring elastic scattering properties. More particularly, Fourier domain, low-coherence interferometry techniques are applied to light scattering spectroscopy. This approach permits the viewing and recovery of depth-resolved structures, as well as obtaining spectroscopic information about scattered light as a function of depth.
2. Background of the Related Art
Accurately measuring small objects or other physical phenomena is a goal that is pursued in many diverse fields of scientific endeavor. For example, in the study of cellular biology and cellular structures, light scattering spectroscopy (LSS) has received much attention recently as a means for probing cellular morphology and the diagnosing of dysplasia. The disclosures of the following references are incorporated by reference in their entirety:
The LSS technique examines variations in the elastic scattering properties of cell organelles to infer their sizes and other dimensional information. In order to measure cellular features in tissues and other cellular structures, it is necessary to distinguish the singly scattered light from diffuse light, which has been multiply scattered and no longer carries easily accessible information about the scattering objects. This distinction or differentiation can be accomplished in several ways, such as the application of a polarization grating, by restricting or limiting studies and analysis to weakly scattering samples, or by using modeling to remove the diffuse component (s).
As an alternative approach for selectively detecting singly scattered light from sub-surface sites, low-coherence interferometry (LCI) has also been explored as a method of LSS. Experimental results have shown that using a broadband light source and its second harmonic allows the recovery of information about elastic scattering using LCI .
More recently, angle-resolved LCI (a/LCI) has demonstrated the capability of obtaining structural information by examining the angular distribution of scattered light from the sample or object under examination. The a/LCI technique has been successfully applied to measuring cellular morphology and to diagnosing intraepithelial neoplasia in an animal model of carcinogenesis.
The above references are incorporated by reference herein where appropriate for appropriate teachings of additional or alternative details, features and/or technical background.
The claimed exemplary embodiments of the present invention address some of the issues presented above.
An object of the invention is to solve at least the above problems and/or disadvantages and to provide at least the advantages described hereinafter.
In one exemplary embodiment of the present invention, an apparatus comprises a first receiver that receives a first reference light and outputs a second reference light. A second receiver that receives a first sample light and outputs a second sample light and wherein the second sample light contains light scattered from a sample when at least a portion of the first sample light is scattered from a sample. A cross-correlator that receives and cross-correlates the second reference light with the second sample light. The cross-correlator may be a spatial cross-correlator.
In another exemplary embodiment of the present invention, a reference arm receives a first reference light and outputs a second reference light. A sample receives a first sample light and outputs a second sample light and wherein the second sample light contains light scattered from the sample when at least a portion of said first sample light is scattered from the sample. A spatial cross-correlator receives and cross correlates the second reference light with the second sample light. The spatial cross-correlator comprises a detector and a processing unit. The detector outputs an interference term to the processing unit. The processing unit processes the interference term to yield depth resolved cross-correlation reflection profiles of the sample. The processing unit first applies a Gaussian window and then a Fourier transform transforms the interference term to yield depth resolved cross-correlation reflection profiles of the sample. The Fourier transform obtains an axial spatial cross-correlation between a signal field(s) and a reference field(s). A light source outputs light, which contains the first sample light and the first reference light.
In another exemplary embodiment of the present invention, a method comprises receiving a first reference light and outputting a second reference light. A first sample light is received and a second sample light is output. The second sample light contains light scattered from a sample when at least a portion of the first sample light is scattered from a sample along with the reception and cross correlation of the second reference light with the second sample light.
In another exemplary embodiment, a method comprises receiving light and splitting at least a portion of the light into reference light and sample light. At least a portion of said reference light is reflected from a reference surface to yield reflected reference light. At least a portion of the sample light is scattered from a sample to yield scattered sample light, and the scattered sample and the reflected reference light are mixed. Information is recovered about the scattered sample light. The mixing comprises detecting an intensity of the scattered sample light and the reflected reference light. Recovering information comprises extracting an interference term from a total intensity. Recovering information can further comprise applying a mathematical operator to the interference term to recover the spectral information about the scattered sample light at a particular depth to yield depth resolved cross-correlation reflection points of the sample. The mathematical operator used is preferably a Gaussian window.
The invention will be described in detail with reference to the following drawings in which like reference numerals refer to like elements wherein:
In the following detailed description of the various exemplary embodiments, reference is made to the accompanying drawings that show, by way of illustration, specific embodiments in which the invention may be practiced. In the drawings, like numerals describe substantially similar components throughout the several views. These embodiments are described in sufficient detail to enable those skilled in the art to practice the invention. Other embodiments may be utilized without departing from the scope of the present invention. Moreover, it is to be understood that various embodiments of the invention, although different, are not necessarily mutually exclusive. For example, a particular feature, structure, or characteristic described in one embodiment may be included within other embodiments. Therefore, the following detailed description is not to be taken in a limiting sense. The scope of the present invention is delineated by the claims, along with the full scope of equivalents to which such claims are entitled.
The contents of the following references are incorporated by reference in their entirety: Wojtkowski, M., A. Kowalczyk, R. Leitgeb, and A. F. Fercher, Opt. Lett., 27(16): p. 1415-1417 (2002); Wojtkowski, M., R. Leitgeb, A. Kowalczyk, T. Bajraszewski, and A. F. Fercher, J. Biomed. Opt., 7(3): p. 457-463 (2002); Leitgeb, R., M. Wojtkowski, A. Kowalczyk, C. K. Hitzenberger, M. Sticker, and A. F. Fercher, Opt. Lett., 25(11): p. 820-822 (2000).
In general, spectral radar makes use of techniques where depth-resolved structural information is recovered by applying a Fourier transform to the spectrum of two mixed fields. In fLCI, the aforementioned approach used in spectral radar applications is extended to recover not only depth-resolved structure, but also to obtain spectroscopic information about scattered light as a function of depth. The capabilities of fLCI enable extracting the size of polystyrene beads in a sub-surface layer based on their light scattering spectrum. The apparatus and method according to exemplary embodiments of the invention can be applied to many different areas. One such area of application is to recover nuclear morphology of sub-surface cell layers.
One exemplary embodiment of the fLCI scheme is shown in
This illumination scheme achieves Kohler illumination in that the fiber acts as a field stop, resulting in the proper alignment of incident or illuminating light and thereby achieving critical illumination of the sample. In the fLCI system 10, the white light beam is split by the beamsplitter 106 (BS) into a reference beam 105 and an input beam 107 to the sample 108. The light scattered by the sample 108 is recombined at the BS 106 with light reflected by the reference mirror 114 (M).
The reference beam 105 in conjunction with the reference mirror 114 forms a portion of a reference arm that receives a first reference light and outputs a second reference light. The input beam 107 and the sample 108 form a portion of a sample arm that receives a first sample light and outputs a second sample light.
Those skilled in the art will appreciate that the light beam can be split into a plurality of reference beams and input beams (e.g. N reference beams and N input beams) without departing from the spirit and scope of the present invention. Further, the splitting of the beams may be accomplished with a beamsplitter or a fiber splitter in the case of an optical fiber implementation of and exemplary embodiment of the present invention.
In the exemplary embodiment of the present invention shown in
The detected signal is linearly related to the intensity as a function of wavelength I(λ), which can be related to the signal and reference fields (Es, Er) as:
<I(λ)>=<|Es(λ)|2>+<|Er(λ)|2>+2Re<Es(λ)E*r(λ)>cos φ (1)
where φ is the phase difference between the two fields and <. . .> denotes an ensemble average.
The interference term is extracted by measuring the intensity of the signal and reference beams independently and subtracting them from the total intensity.
The axial spatial cross-correlation function, ΓSR(z) between the sample and reference fields is obtained by resealing the wavelength spectrum into a wavenumber (k=2π/λ) spectrum then Fourier transforming:
ΓSR(z)=∫dkeikz<Es(k)E*r(k)>cos φ. (2)
This term is labeled as an axial spatial cross-correlation as it is related to the temporal or longitudinal coherence of the two fields.
Another exemplary embodiment of an fLCI scheme is shown in
The reference light in reference fiber 125, in conjunction with a lens 126 (preferably an aspheric lens) and the reference mirror 128, forms a portion of a reference arm that receives a first reference light and outputs a second reference light. Specifically, reference light in reference fiber 125 is directed to the reference mirror 128 by lens 126, and the reference light reflected by the reference mirror 128 (second reference light) is coupled back into the reference fiber 125 with lens 126. The sample light in sample fiber 127 and the sample 130 form a portion of a sample arm that receives a first sample light and outputs a second sample light. Specifically, sample light in sample fiber 127 is directed to the sample 130 by lens 131 (preferably as aspheric lens), and at least a portion of the sample light scattered by the sample 130 is coupled into the sample fiber 127 by lens 131. In the exemplary embodiment shown in
At least a portion of the reflected reference light in reference fiber 125 and at least a portion of the scattered sample light on sample fiber 127 are coupled into a detector fiber 133 by the FS 124.
The output of detector fiber 133 coincides with the input of a miniature spectrograph 132, where the light is spectrally dispersed and detected.
From this autocorrelation, the coherence length of the field, lc=1.21 μm is determined. This is slightly larger than the calculated width of lc=2/Δkl/c=0.98 μm, with any discrepancy most likely attributed to uncompensated dispersion effects. Note that rescaling the field into wavenumber space is a nonlinear process which can skew the spectrum if not properly executed .
In data processing, a fitting algorithm is applied (e.g. a cubic spline fit) to the rescaled wavenumber spectrum and then resampled (e.g. resample with even spacing). The resampled spectrum is then Fourier transformed to yield the spatial correlation of the sample. Those skilled in the art will appreciate that other frequency based algorithms or combinations of algorithms can be used in place of the Fourier transform to yield spatial correlation. One example of a software tool that can be used to accomplish this processing in real time or near real time is to use LabView™ software.
In one exemplary embodiment of the present invention, the sample consists of a glass coverslip (e.g., thickness, d˜200 μm) with polystyrene beads which have been dried from suspension onto the back surface (1.55 μm mean diameter, 3% variance). Thus, the field scattered by the sample can be expressed as:
In equation 3, Efront and Eback denote the field scattered by the front and back surfaces of the coverslip, and δz is the difference between the path length of the reference beam and that of the light reflected from the front surface and n the index of refraction of the glass. The effect of the microspheres will appear in the Eback term as the beads are small and attached closely to the back surface. Upon substituting equation 3 into equation 2, a two peak distribution with the width of the peaks given by the coherence length of the source is obtained.
In order to obtain spectroscopic information, a Gaussian window is applied to the interference term before performing the Fourier transform operation. Those skilled in the art will appreciate that other probabilistic windowing methodologies may be applied without departing from the spirit and scope of the invention. This makes it possible to recover spectral information about light scattered at a particular depth.
The windowed interference term takes the form:
<Es(k)E*r(k)>exp [−((k−kw)/Δkw)2]. (4)
The proper sizing of a windowed interference term can facilitate the processing operation. For example, by selecting a relatively narrow window (Δkw small) compared to the features of Es and Ek, we effectively obtain <Es(kw)E*r(kw) >. In processing the data below, we use Δkw=0.12 μm−1 which degrades the coherence length by a factor of 16.7. This exemplary window setting enables the scattering at 50 different wavenumbers over the 6 μm−1 span of usable spectrum.
Note that the correlation function is symmetric about z=0, resulting in a superposed mirror image of the scan. Since these are represented as cross-correlation functions, the plots are symmetric about z=0. Thus the front surface reflection for z>0 is paired with the back surface reflection for z<0, and vice versa.
To obtain the spectrum of the scattered light, we repeatedly apply the Gaussian window and increase the center wavenumber by 0.12 μm−1 between successive applications. As mentioned above, Δkw=0.12 μm−1 is used to degrade the coherence length by a factor of 16.7. This results in the generation of a spectroscopic depth-resolved reflection profile.
For comparison, the same ratio for the front surface reflections (dashed line in
There are many applications of the various exemplary embodiments of the present invention. One exemplary application of fLCI is in determining the size of cell organelles, in particular the cell nucleus, in epithelial tissues. In biological media, for example, the relative refractive indices are lower for organelles compared to microspheres and thus, smaller scattering signals are expected. The use of a higher power light source will permit the smaller signals to be detected. Other examples include detection of sub-surface defects in manufactured parts, including fabricated integrated circuits, detection of airborne aerosols, such as nerve agents or biotoxins, and detection of exposure to such aerosols by examining epithelial tissues within the respiratory tract.
Additionally, the larger the size of the nucleus (compared to the microspheres in this experiment), the higher the frequency modulation of the spectrum. Those skilled in the art will appreciate that higher frequency oscillations are detected at a lower efficiency in Fourier transform spectroscopy techniques. Therefore, in order to detect these higher frequency oscillations, a higher resolution spectrograph is used.
The foregoing example illustrates how the exemplary embodiments of the present invention can be modified in various manners to improve performance in accordance with the spirit and scope of the present invention.
From the foregoing detailed description, it should be apparent that fLCI can recover structural information with sub-wavelength accuracy from sub-surface layers based on measuring elastic scattering properties. The simplicity of the system makes it an excellent candidate for probing cellular morphology in tissue samples and may one day serve as the basis for a biomedical diagnostic device.
The foregoing embodiments and advantages are merely exemplary and are not to be construed as limiting the present invention. The present teaching can be readily applied to other types of apparatuses. The description of the present invention is intended to be illustrative, and not to limit the scope of the claims. Many alternatives, modifications, and variations will be apparent to those skilled in the art. In the claims, means-plus-function clauses are intended to cover the structures described herein as performing the recited function and not only structural equivalents but also equivalent structures.
|Cited Patent||Filing date||Publication date||Applicant||Title|
|US4646722||Dec 10, 1984||Mar 3, 1987||Opielab, Inc.||Protective endoscope sheath and method of installing same|
|US5386817||Apr 5, 1993||Feb 7, 1995||Endomedical Technologies, Inc.||Endoscope sheath and valve system|
|US5489256||Nov 2, 1994||Feb 6, 1996||Adair; Edwin L.||Sterilizable endoscope with separable disposable tube assembly|
|US5534707||Oct 8, 1992||Jul 9, 1996||Beckman Instruments, Inc.||Apparatus and method for aligning capillary column and detection optics|
|US5565986||Mar 16, 1995||Oct 15, 1996||Kn+E,Uml U+Ee Ttel; Alexander||Stationary optical spectroscopic imaging in turbid objects by special light focusing and signal detection of light with various optical wavelengths|
|US5601087||Jun 7, 1995||Feb 11, 1997||Spectrascience, Inc.||System for diagnosing tissue with guidewire|
|US5643175||Feb 5, 1996||Jul 1, 1997||Adair; Edwin L.||Sterilizable endoscope with separable disposable tube assembly|
|US5771327||Nov 18, 1996||Jun 23, 1998||Optical Biopsy||Optical fiber probe protector|
|US5930440||Feb 18, 1998||Jul 27, 1999||Optical Biopsy Technologies, Llc||Fiber optic probe protector|
|US5956355 *||Jun 17, 1997||Sep 21, 1999||Massachusetts Institute Of Technology||Method and apparatus for performing optical measurements using a rapidly frequency-tuned laser|
|US6002480 *||Jun 2, 1998||Dec 14, 1999||Izatt; Joseph A.||Depth-resolved spectroscopic optical coherence tomography|
|US6091984||Oct 10, 1997||Jul 18, 2000||Massachusetts Institute Of Technology||Measuring tissue morphology|
|US6134003 *||Feb 27, 1996||Oct 17, 2000||Massachusetts Institute Of Technology||Method and apparatus for performing optical measurements using a fiber optic imaging guidewire, catheter or endoscope|
|US6174291||Mar 9, 1998||Jan 16, 2001||Spectrascience, Inc.||Optical biopsy system and methods for tissue diagnosis|
|US6233373||Jun 21, 1999||May 15, 2001||The United States Of America As Represented By The Secretary Of The Navy||Optical spectrometer with improved geometry and data processing for monitoring fiber optic bragg gratings|
|US6263133||Mar 24, 2000||Jul 17, 2001||Scimed Life Systems, Inc.||Optical focusing, collimating and coupling systems for use with single mode optical fiber|
|US6404497||Jan 25, 1999||Jun 11, 2002||Massachusetts Institute Of Technology||Polarized light scattering spectroscopy of tissue|
|US6501551||Oct 5, 1999||Dec 31, 2002||Massachusetts Institute Of Technology||Fiber optic imaging endoscope interferometer with at least one faraday rotator|
|US6564087||Jul 22, 1999||May 13, 2003||Massachusetts Institute Of Technology||Fiber optic needle probes for optical coherence tomography imaging|
|US6624890||May 24, 2002||Sep 23, 2003||Massachusetts Institute Of Technology||Polarized light scattering spectroscopy of tissue|
|US6697652||Jan 19, 2001||Feb 24, 2004||Massachusetts Institute Of Technology||Fluorescence, reflectance and light scattering spectroscopy for measuring tissue|
|US6775007||Jan 29, 2002||Aug 10, 2004||Joseph A. Izatt||Frequency-encoded parallel OCT and associated systems and methods|
|US6847456||Apr 27, 2001||Jan 25, 2005||Massachusetts Institute Of Technology||Methods and systems using field-based light scattering spectroscopy|
|US6853457||Sep 4, 2001||Feb 8, 2005||Forskningscenter Riso||Optical amplification in coherence reflectometry|
|US6863651||Oct 19, 2001||Mar 8, 2005||Visionscope, Llc||Miniature endoscope with imaging fiber system|
|US6879741||Nov 4, 2002||Apr 12, 2005||C Technologies, Inc||Sampling end for fiber optic probe|
|US7061622||Aug 5, 2002||Jun 13, 2006||Case Western Reserve University||Aspects of basic OCT engine technologies for high speed optical coherence tomography and light source and other improvements in optical coherence tomography|
|US7079254||Mar 18, 2004||Jul 18, 2006||Southwest Sciences Incorporated||Method and apparatus for imaging internal structures of transparent and translucent materials|
|US7102758||May 6, 2003||Sep 5, 2006||Duke University||Fourier domain low-coherence interferometry for light scattering spectroscopy apparatus and method|
|US7355716||Jan 24, 2003||Apr 8, 2008||The General Hospital Corporation||Apparatus and method for ranging and noise reduction of low coherence interferometry LCI and optical coherence tomography OCT signals by parallel detection of spectral bands|
|US7366372||Feb 27, 2006||Apr 29, 2008||Honeywell International, Inc.||Waveguide device having improved spatial filter configurations|
|US7391520||Jul 1, 2005||Jun 24, 2008||Carl Zeiss Meditec, Inc.||Fourier domain optical coherence tomography employing a swept multi-wavelength laser and a multi-channel receiver|
|US7417740||Nov 12, 2004||Aug 26, 2008||Medeikon Corporation||Single trace multi-channel low coherence interferometric sensor|
|US7428050||May 13, 2004||Sep 23, 2008||The University Of Akron||Multispectral, multifusion, laser-polarimetric optical imaging system|
|US7428052||Dec 8, 2005||Sep 23, 2008||Fujinon Corporation||Optical tomographic apparatus|
|US7616323||Jan 19, 2006||Nov 10, 2009||Zygo Corporation||Interferometer with multiple modes of operation for determining characteristics of an object surface|
|US7633627||Jan 20, 2006||Dec 15, 2009||Duke University||Methods, systems and computer program products for characterizing structures based on interferometric phase data|
|US7636168||Oct 11, 2006||Dec 22, 2009||Zygo Corporation||Interferometry method and system including spectral decomposition|
|US7761139||Jan 26, 2004||Jul 20, 2010||The General Hospital Corporation||System and method for identifying tissue using low-coherence interferometry|
|US20020143243||Jan 19, 2001||Oct 3, 2002||Massachusetts Institute Of Technology||Fluorescence, reflectance and light scattering spectroscopy for measuring tissue|
|US20020171831||May 24, 2002||Nov 21, 2002||Massachusetts Institute Of Technology||Polarized light scattering spectroscopy of tissue|
|US20030042438||Aug 31, 2001||Mar 6, 2003||Lawandy Nabil M.||Methods and apparatus for sensing degree of soiling of currency, and the presence of foreign material|
|US20030137669||Aug 5, 2002||Jul 24, 2003||Rollins Andrew M.||Aspects of basic OCT engine technologies for high speed optical coherence tomography and light source and other improvements in optical coherence tomography|
|US20040215296||Jan 9, 2004||Oct 28, 2004||Barrx, Inc.||System and method for treating abnormal epithelium in an esophagus|
|US20040223162||May 6, 2003||Nov 11, 2004||Duke University||Fourier domain low-coherence interferometry for light scattering spectroscopy apparatus and method|
|US20050004453||Jan 26, 2004||Jan 6, 2005||Tearney Guillermo J.||System and method for identifying tissue using low-coherence interferometry|
|US20050053974||May 20, 2004||Mar 10, 2005||University Of Maryland||Apparatus and methods for surface plasmon-coupled directional emission|
|US20060132790||Feb 17, 2004||Jun 22, 2006||Applied Science Innovations, Inc.||Optical coherence tomography with 3d coherence scanning|
|US20060158657||Jan 19, 2006||Jul 20, 2006||De Lega Xavier C||Interferometer for determining characteristics of an object surface, including processing and calibration|
|US20060164643||May 13, 2004||Jul 27, 2006||Giakos George C||Multispectral, multifusion, laser-polarimetric optical imaging system|
|US20060256343||Jan 20, 2006||Nov 16, 2006||Michael Choma||Methods, systems and computer program products for characterizing structures based on interferometric phase data|
|US20060285635||Apr 14, 2006||Dec 21, 2006||Boppart Stephen A||Contrast enhanced spectroscopic optical coherence tomography|
|US20070002327||Jul 1, 2005||Jan 4, 2007||Yan Zhou||Fourier domain optical coherence tomography employing a swept multi-wavelength laser and a multi-channel receiver|
|US20070015969||Jun 5, 2006||Jan 18, 2007||Board Of Regents, The University Of Texas System||OCT using spectrally resolved bandwidth|
|US20070027391||Jul 27, 2006||Feb 1, 2007||Fujinon Corporation||Optical diagnosis and treatment apparatus|
|US20070086013||Oct 11, 2006||Apr 19, 2007||Zygo Corporation||Interferometry method and system including spectral decomposition|
|US20070133002||Oct 11, 2006||Jun 14, 2007||Duke University||Systems and methods for endoscopic angle-resolved low coherence interferometry|
|US20070165234||Oct 14, 2004||Jul 19, 2007||University Of Kent||Spectral interferometry method and apparatus|
|US20070201033||Feb 21, 2007||Aug 30, 2007||The General Hospital Corporation||Methods and systems for performing angle-resolved fourier-domain optical coherence tomography|
|US20080037024||May 11, 2007||Feb 14, 2008||Vadim Backman||Systems, methods, and apparatuses of low-coherence enhanced backscattering spectroscopy|
|US20080058629||Aug 21, 2006||Mar 6, 2008||University Of Washington||Optical fiber scope with both non-resonant illumination and resonant collection/imaging for multiple modes of operation|
|US20080249369||Apr 5, 2007||Oct 9, 2008||University Of Washington||Compact scanning fiber device|
|US20080255461||Mar 26, 2008||Oct 16, 2008||Robert Weersink||Real-time optical monitoring system and method for thermal therapy treatment|
|US20090009759||May 14, 2007||Jan 8, 2009||Vadim Backman||Systems, methods and apparatuses of elastic light scattering spectroscopy and low coherence enhanced backscattering spectroscopy|
|US20090075391||Jun 30, 2008||Mar 19, 2009||Newton Laboratories, Inc.||Spectroscopic diagnostic method and system based on scattering of polarized light|
|EP0243005A2||Mar 24, 1987||Oct 28, 1987||Dolan-Jenner Industries, Inc.||Fiber optic imaging system for on-line monitoring|
|EP1021126B1||Oct 9, 1998||Jul 28, 2004||Massachusetts Institute Of Technology||Method for measuring tissue morphology|
|WO1999018845A1||Oct 9, 1998||Apr 22, 1999||Massachusetts Institute Of Technology||Method for measuring tissue morphology|
|WO2000042912A1||Jan 25, 2000||Jul 27, 2000||Massachusetts Institute Of Technology||Polarized light scattering spectroscopy of tissue|
|WO2007133684A2||May 11, 2007||Nov 22, 2007||Northwestern University||Systems, methods, and apparatuses of low-coherence enhanced backscattering spectroscopy|
|1||Amoozegar, Cyrus et a., "Experimental Verification of T-matrix-based Inverse Light Scattering Analysis for Assessing Structure of Spheroids as Models of Cell Nuclei," Applied Optics, vol. 48, No. 10, to be published Apr. 1, 2009, 7 pages.|
|2||Backman, V. et al., "Detection of Preinvasive Cancer Cells," Nature 406, Jul. 6, 2000, pp. 35-36.|
|3||Backman, V. et al., "Measuring Cellular Structure at Submicrometer Scale with Light Scattering Spectroscopy," IEEE J. Sel. Top. Quantum Electron, vol. 7, Issue 6, Nov./Dec. 2001, pp. 887-893.|
|4||Brown, William J. et al., "Review and Recent Development of Angle-Resolved Low-Coherence Interferometry for Detection of Precancerous Cells in Human Esophageal Epithelium," IEEE Journal of Selected Topics in Quantum Electronics, vol. 14, No. 1, Jan./Feb. 2008, pp. 88-97.|
|5||Chalut, Kevin J. et al., "Application of Mie Theory to Assess Structure of Spheroidal Scattering in Backscattering Geometries," J. Opt. Soc. Am. A, vol. 25, No. 8, Aug. 2008, pp. 1866-1874.|
|6||Chalut, Kevin J., et al., "Label-Free, High-Throughput Measurements of Dynamic Changes in Cell Nuclei Using Angle-Resolved Low Coherence Interferometry," Biophysical Journal, vol. 94, Jun. 2008, pp. 4948-4956.|
|7||Choma, Michael A. et al., "Sensitivity Advantage of Swept Source and Fourier Domain Optical Coherence Tomography," Optics Express, vol. 11, No. 18, Sep. 8, 2003, pp. 2183-2189.|
|8||de Boer, Johannes F. et al., "Improved Signal-To-Noise Ratio in Spectral-Domain Compared with Time-Domain Optical Coherence Tomography," Optics Letters, vol. 28, No. 21, Nov. 1, 2003, pp. 2067-2069, http://oa.osa.org/abstract.cfm?id=86605.|
|9||Giacomelli, Michael G. et al., "Application of the T-matrix Method to Determine the Structure of Spheroidal Cell Nuclei with Angle-resolved Light Scattering," Optics Letters, vol. 33, No. 21, Nov. 1, 2008, pp. 2452-2454.|
|10||Graf, R. N. et al., "Parallel Frequency-Domain Optical Coherence Tomography Scatter-Mode Imaging of the Hamster Cheek Pouch Using a Thermal Light Source," Optics Letters, vol. 33, No. 12, Jun. 15, 2008, pp. 1285-1287.|
|11||Hausler, G. et al., "Coherence Radar and Spectral Radar-New Tools for Dermatological Diagnosis," Journal of Biomedical Optics, vol. 3, Jan. 1998.|
|12||Hausler, G. et al., "Coherence Radar and Spectral Radar—New Tools for Dermatological Diagnosis," Journal of Biomedical Optics, vol. 3, Jan. 1998.|
|13||Keener, Justin D. et al., "Application of Mie Theory to Determine the Structure of Spheroidal Scatterers in Biological Materials," Optics Letters, vol. 32, No. 10, May 15, 2007, pp. 1326-1328.|
|14||Kim, Y.L. et al., "Simultaneous Measurement of Angular and Spectral Properties of Light Scattering for Characterization of Tissue Microarchitecture and its Alteration in Early Precancer," IEEE Journal of Selected Topics in Quantum Electronics, vol. 9, Issue 2, Mar./Apr. 2003, pp. 243-256, http://ieeexploreieee-org/xpl/freeabs-all.jsp?tp=&arnumber=1238988&isnumber=27791.|
|15||Kim, Y.L. et al., "Simultaneous Measurement of Angular and Spectral Properties of Light Scattering for Characterization of Tissue Microarchitecture and its Alteration in Early Precancer," IEEE Journal of Selected Topics in Quantum Electronics, vol. 9, Issue 2, Mar./Apr. 2003, pp. 243-256, http://ieeexploreieee—org/xpl/freeabs—all.jsp?tp=&arnumber=1238988&isnumber=27791.|
|16||Leitgeb, R. et al., "Performance of Fourier Domain vs. Time Domain Optical Coherence Tomography," Optics Express, vol. 11, No. 8, Apr. 21, 2003, pp. 889-894.|
|17||Leitgeb, R. et al., "Spectral Measurement of Absorption by Spectroscopic Frequency-Domain Optical Coherence Tomography," Optic Letters, vol. 25, Issue 11, Jun. 1, 2000, pp. 820-822.|
|18||Morgner, U. et al., "Spectroscopic Optical Coherence Tomography," Optic Letters, vol. 25, Issue 2, Jan. 15, 2000, pp. 111-113.|
|19||Pyhtila, John W. et al., "Coherent Light Scattering by In Vitro Cell Arrays Observed with Angle-Resolved Low Coherence Interferometry," SPIE, vol. 5690, 2005.|
|20||Pyhtila, John W. et al., "Determining Nuclear Morphology Using an Improved Angle-Resolved Low Coherence. Interferometry System," Optics Express, vol. 11, No. 25, Dec. 15, 2003.|
|21||Pyhtila, John W. et al., "Fourier-Domain Angle-Resolved Low Coherence Interferometry Through an Endoscopic Fiber Bundle for Light-Scattering Spectroscopy," Optic Letters, vol. 31, No. 6, Mar. 15, 2006.|
|22||Pyhtila, John W. et al., "Polarization Effects on Scatterer Sizing Accuracy Analyzed with Frequency-Domain Angle-Resolved Low-Coherence Interferometry," Applied Optics, vol. 46, No. 10, Apr. 1, 2007.|
|23||Pyhtila, John W. et al., "Rapid, Depth-Resolved Light Scattering Measurements using Fourier Domain, Angle-Resolved Low Coherence Interferometry," Optics Express, vol. 12, No. 25, Dec. 13, 2004.|
|24||Robles, Francisco et al., "Dual Window Method for Processing Spectroscopic OCT Signals with Simultaneous High Spectral and Temporal Resolution," Optical Society of America, 2008, 12 pages.|
|25||Roy, Hemant K. et al., "Four-Dimensional Elastic Light-Scattering Fingerprints as Preneoplastic Markers in the Rat Model of Colon Carcinogenesis," Gastroenterology, vol. 126, Issue 4, Apr. 2004, pp. 1071-1081, http://www.gastrojoumal.org/article/PIIS0016508501000290/abstract.|
|26||Tuchin, V. et al., Tissue Optics: Light Scattering Methods and Instruments for Medical Diagnosis, SPIE, May 2000.|
|27||Wax, Adam et al., "Angular Light Scattering Studies Using Low-Coherence Interferometry," SPIE, vol. 4251, 2001.|
|28||Wax, Adam et al., "Cellular Organization and Substructure Measured Using Angle-Resolved Low-Coherence Interferometry," Biophysical Journal, Apr. 2002, pp. 2256-2264, vol. 82.|
|29||Wax, Adam et al., "Determination of Particle Size Using the Angular Distribtion of Backscattered Light as Measured with Low-Coherence Interferometry," Journal of the Optical Society of America, Apr. 2002, pp. 737-744, vol. 19, No. 4.|
|30||Wax, Adam et al., "Fourier-Domain Low-Coherence Interferometry for Light-Scaterring Spectroscopy," Optic Letters, vol. 28, No. 14, Jul. 15, 2003, pp. 1230-1232.|
|31||Wax, Adam et al., "In Situ Detection of Neoplastic Transformation and Chemopreventive Effects in Rat Esophagus Epithelium Using Angle-Resolved Low-Coherence Interferometry," Cancer Research, Jul. 1, 2003, pp. 3556-3559, vol. 63, No. 13.|
|32||Wax, Adam et al., "Measurement of Angular Distributions by Use of Low-Coherence Interferometry for Light-Scattering Spectroscopy," Optics Letters, Mar. 15, 2001, pp. 322-324, vol. 26, No. 6.|
|33||Wax, Adam et al., "Prospective Grading of Neoplastic Change in Rat Esophagus Epithelium Using Angle-Resolved Low-Coherence Interferometry," Journal of Biomedical Optics, vol. 10(5), Sep./Oct. 2005, pp. 051604-1 through 051604-10.|
|34||Wax, Adam, "Studying the Living Cell Using Light Scattering and Low-Coherence Interferometry," Laser Biomedical Research Center, MIT Spectroscopy Laboratory, presented at Case Western Reserve University 2002, Feb. 1, 2002.|
|35||Wojtkowski, M. et al., "Full Range Complex Spectral Optical Coherence Tomography Technique in Eye Imaging ," Optics Letters, vol. 27, Issue 16, Aug. 15, 2002, pp. 1415-1417.|
|36||Wojtkowski, M. et al., "In Vivo Human Retinal Imaging by Fourier Domain Optical Coherence Tomography," J. Biomed. Opt., vol. 7, No. 3, Jul. 1, 2002, pp. 457-463.|
|37||Xie, Tuqiang et al., "Fiber-Optic-Bundle-Based Optical Coherehence Tomography," Optic Letters, vol. 30, No. 14, Jul. 15, 2005.|
|Citing Patent||Filing date||Publication date||Applicant||Title|
|US8233152 *||Jul 9, 2009||Jul 31, 2012||Canon Kabushiki Kaisha||Optical coherence tomographic imaging method and optical coherence tomographic imaging apparatus|
|US8836952||Jun 19, 2012||Sep 16, 2014||Canon Kabushiki Kaisha||Optical coherence tomographic imaging method and optical coherence tomographic imaging apparatus|
|US9274001 *||Jan 24, 2011||Mar 1, 2016||Duke University||Dual window processing schemes for spectroscopic optical coherence tomography (OCT) and fourier domain low coherence interferometry|
|US20100027019 *||Jul 9, 2009||Feb 4, 2010||Canon Kabushiki Kaisha||Optical Coherence Tomographic Imaging Method and Optical Coherence Tomographic Imaging Apparatus|
|US20130135614 *||Jan 24, 2011||May 30, 2013||Adam Wax||Dual window processing schemes for spectroscopic optical coherence tomography (oct) and fourier domain low coherence interferometry|
|WO2014144307A2||Mar 14, 2014||Sep 18, 2014||Gebhart Steven C||Probe assembly and disposable cover particularly for use in endoscope applications of low coherence interferometry|
|International Classification||G01B9/02, G01N15/02|
|Sep 20, 2011||CC||Certificate of correction|
|Feb 6, 2014||FPAY||Fee payment|
Year of fee payment: 8