Optical Non-Invasive Approaches to Diagnosis of Skin Diseases

Slides:



Advertisements
Similar presentations
Spectral Resolution and Spectrometers
Advertisements

Spectral Resolution and Spectrometers A Brief Guide to Understanding and Obtaining the Proper Resolution of the 785 Raman System.
OPTICS. I. IMAGES A. Definition- An image is formed where light rays originating from the same point on an object intersect on a surface or appear to.
R. Hui Photonics for bio-imaging and bio- sensing Rongqing Hui Dept. Electrical Engineering & Computer Science, The University of Kansas, Lawrence Kansas.
Optical Coherence Tomography Zhongping Chen, Ph.D. Optical imaging in turbid media Coherence and interferometry Optical coherence.
© 2010 Pearson Education, Inc. Conceptual Physics 11 th Edition Chapter 28: REFLECTION & REFRACTION Reflection Principle of Least Time Law of Reflection.
5 Components Common to All Optical Spectrometers Source Transparent Sample Holder Wavelength Selector Radiation Detector Signal Processor and Readout.
Chapter 24 Wave Optics. General Physics Review – waves T=1/f period, frequency T=1/f period, frequency v = f velocity, wavelength v = f velocity, wavelength.
L 33 Light and Optics [4] Measurements of the speed of light  The bending of light – refraction  Total internal reflection  Dispersion Dispersion 
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Index-matching effect. Matching the index of refraction of the bead with the solution.
Date of download: 6/22/2016 Copyright © 2016 SPIE. All rights reserved. Prismless confocal total internal reflection (CTIR) microscope. 532-nm light is.
Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. (a) Cartoon of flip-chip InGaAs FPA with InP substrate. SWIR light passes through.
Date of download: 7/8/2016 Copyright © 2016 SPIE. All rights reserved. Through-the-objective TIRF creates the evanescent field on the aqueous side of the.
Phys102 Lecture 26, 27, 28 Diffraction of Light Key Points Diffraction by a Single Slit Diffraction in the Double-Slit Experiment Limits of Resolution.
Date of download: 9/18/2016 Copyright © 2016 SPIE. All rights reserved. Schematic of the simultaneous time- and wavelength resolved fluorescence spectroscopy.
Refraction and Lenses.
Optical Non-Invasive Approaches to Diagnosis of Skin Diseases
Optical biopsy: A new frontier in endoscopic detection and diagnosis
Volume 102, Issue 3, Pages (February 2012)
Chapter 35-Diffraction Chapter 35 opener. Parallel coherent light from a laser, which acts as nearly a point source, illuminates these shears. Instead.
P.J. Caspers, G.W. Lucassen, G.J. Puppels  Biophysical Journal 
Volume 102, Issue 3, Pages (February 2012)
Demarcation of Nonmelanoma Skin Cancer Margins in Thick Excisions Using Multispectral Polarized Light Imaging  Anna N. Yaroslavsky, Victor Neel, R. Rox.
Optical biopsy: A new frontier in endoscopic detection and diagnosis
Volume 84, Issue 6, Pages (June 2003)
Tissa R. Hata, Theresa A. Scholz, Lynn K. Pershing 
Volume 97, Issue 4, Pages (August 2009)
L 34 Light and Optics [4] Measurements of the speed of light 
Dual Mode Reflectance and Fluorescence Confocal Laser Scanning Microscopy for In Vivo Imaging Melanoma Progression in Murine Skin  Yanyun Li, Salvador.
Imaging Structural Proteins
Volume 56, Issue 2, Pages (August 2009)
The Mobility of Phytochrome within Protonemal Tip Cells of the Moss Ceratodon purpureus, Monitored by Fluorescence Correlation Spectroscopy  Guido Böse,
In Vivo Confocal Scanning Laser Microscopy of Human Skin II: Advances in Instrumentation and Comparison With Histology1  Milind Rajadhyaksha, Salvador.
LIGHT MICROSCOPY variations
Volume 95, Issue 7, Pages (October 2008)
Volume 83, Issue 6, Pages (December 2002)
In Vivo Confocal Raman Microspectroscopy of the Skin: Noninvasive Determination of Molecular Concentration Profiles  Peter J. Caspers, Hajo A. Bruining,
Sapun H. Parekh, Young Jong Lee, Khaled A. Aamer, Marcus T. Cicerone 
Orientation of the Infrared Transition Moments for an α-Helix
Philippe Hallégot  Journal of Investigative Dermatology 
Cylindrical Illumination Confocal Spectroscopy: Rectifying the Limitations of Confocal Single Molecule Spectroscopy through One-Dimensional Beam Shaping 
L 34 Light and Optics [4] Measurements of the speed of light 
Noninvasive Imaging of Melanoma with Reflectance Mode Confocal Scanning Laser Microscopy in a Murine Model  Daniel S. Gareau, Glenn Merlino, Christopher.
Scanning Near-Field Fluorescence Resonance Energy Transfer Microscopy
Supraresolution Imaging in Brain Slices using Stimulated-Emission Depletion Two- Photon Laser Scanning Microscopy  Jun B. Ding, Kevin T. Takasaki, Bernardo.
Volume 114, Issue 4, Pages (February 2018)
Confocal Examination of Nonmelanoma Cancers in Thick Skin Excisions to Potentially Guide Mohs Micrographic Surgery Without Frozen Histopathology  Milind.
A Comparative Study of Photoacoustic and Reflectance Methods for Determination of Epidermal Melanin Content  John A. Viator, Jason Komadina, Lars O. Svaasand,
Imaging Melanoma in a Murine Model Using Reflectance-Mode Confocal Scanning Laser Microscopy and Polarized Light Imaging  Daniel S. Gareau, James Lagowski,
Endogenous Skin Fluorescence is a Good Marker for Objective Evaluation of Comedolysis  Salvador González, George Zonios, Bach Cuc Nguyen, Robert Gillies,
FLUORESCENCE MICROSCOPY
Bassel H. Mahmoud, Eduardo Ruvolo, Camile L
Volume 104, Issue 1, Pages (January 2013)
Volume 106, Issue 2, Pages (January 2014)
Samuel T. Hess, Watt W. Webb  Biophysical Journal 
Electron Diffraction Provides New Information on Human Stratum Corneum Lipid Organization Studied in Relation to Depth and Temperature  Gonneke S.K. Pilgram,
Attenuated Total Reflection–Fourier Transform Infrared Spectroscopy as a Possible Method to Investigate Biophysical Parameters of Stratum Corneum In Vivo 
Characterization of the Photoconversion on Reaction of the Fluorescent Protein Kaede on the Single-Molecule Level  P.S. Dittrich, S.P. Schäfer, P. Schwille 
Georgios N. Stamatas, Jeff Wu, Nikiforos Kollias 
A Pulsed Electric Field Enhances Cutaneous Delivery of Methylene Blue in Excised Full- Thickness Porcine Skin  Patricia G. Johnson, Stephen A. Gallo, Sek.
P.J. Caspers, G.W. Lucassen, G.J. Puppels  Biophysical Journal 
In Vitro Visualization and Quantification of Oleic Acid Induced Changes in Transdermal Transport Using Two-Photon Fluorescence Microscopy  Betty Yu, Daniel.
Polarized Fluorescence Resonance Energy Transfer Microscopy
Volume 106, Issue 5, Pages (March 2014)
Melanoma Diagnosis by Raman Spectroscopy and Neural Networks: Structure Alterations in Proteins and Lipids in Intact Cancer Tissue  Monika Gniadecka,
Spectral Responses of Melanin to Ultraviolet A Irradiation
Georgios N. Stamatas, Michael Southall, Nikiforos Kollias 
Robert Bissonnette  Journal of Investigative Dermatology 
Volume 91, Issue 4, Pages (August 2006)
The Mobility of Phytochrome within Protonemal Tip Cells of the Moss Ceratodon purpureus, Monitored by Fluorescence Correlation Spectroscopy  Guido Böse,
Presentation transcript:

Optical Non-Invasive Approaches to Diagnosis of Skin Diseases Nikiforos Kollias, Georgios N. Stamatas  Journal of Investigative Dermatology Symposium Proceedings  Volume 7, Issue 1, Pages 64-75 (December 2002) DOI: 10.1046/j.1523-1747.2002.19635.x Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions

Figure 1 Schematic diagram of a confocal arrangement. Light from a laser source passes through a pinhole aperture and is focused in the sample. The point of light focus can scan the sample at different depths by means of moving the objective lens on its longitudinal axis. A second pinhole aperture is placed in a conjugate position to the first pinhole aperture in front of the detector to exclude all out-of-focus information. An image is formed at each depth within the sample by scanning the focus of the incident light in a plane parallel to the surface of the sample. Journal of Investigative Dermatology Symposium Proceedings 2002 7, 64-75DOI: (10.1046/j.1523-1747.2002.19635.x) Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions

Figure 2 Schematic diagram of an interferometric arrangement for OCT. Light from the source passes through a beam-splitter. Half of the light is focused on the sample and half hits a moving mirror. The reflected light from the sample is combined with the reflected light from the mirror and the interference pattern imaged on the detector is analyzed. The depth is probed by analyzing the interference pattern as a function of the position of the moving mirror. The beam that impinges on the sample may then be scanned to obtain an image of position along the sample versus depth – such an image is similar to a histologic section at low resolution (≈13 mm). Journal of Investigative Dermatology Symposium Proceedings 2002 7, 64-75DOI: (10.1046/j.1523-1747.2002.19635.x) Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions

Figure 3 Schematic diagram of an imaging system using filters. Filter 1 can be a bandpass filter or a polarizer. Filter 2 can be a bandpass filter, an LCTF, or a polarizer (positioned either parallel or perpendicular to filter 1). In the case of three-dimensional imaging a fringe pattern projector is in the place of filter 1. Journal of Investigative Dermatology Symposium Proceedings 2002 7, 64-75DOI: (10.1046/j.1523-1747.2002.19635.x) Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions

Figure 4 Schematic diagram of a diffuse reflectance spectrometer. Light illumination is delivered on the skin site of interest by means of an optical fiber bundle. Diffusely reflected light is collected by another set of fibers and is analyzed in terms of its chromatic components or constituent chromophores (color absorbing substances). Journal of Investigative Dermatology Symposium Proceedings 2002 7, 64-75DOI: (10.1046/j.1523-1747.2002.19635.x) Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions

Figure 5 Typical DRS spectrum of an erythematous lesion. Spectral data were obtained with a diffuse reflectance spectrometer from a skin site with a slight erythema normalized to a white standard. The spectrum is decomposed into its component spectra of oxyhemoglobin, deoxyhemoglobin, and melanin. Concentrations of each substance may be estimated from the individual contribution. Journal of Investigative Dermatology Symposium Proceedings 2002 7, 64-75DOI: (10.1046/j.1523-1747.2002.19635.x) Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions

Figure 6 Schematic diagram of a fluorescence spectrometer. Light is delivered and collected from the skin site of interest with an optical fiber bundle. Double monochromators at the illumination and at the detection end allow for sensitive narrow-band excitation and emission. The monochromators can be controlled to sequentially scan the excitation or the emission or both synchronously. Journal of Investigative Dermatology Symposium Proceedings 2002 7, 64-75DOI: (10.1046/j.1523-1747.2002.19635.x) Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions

Figure 7 Typical fluorescence excitation spectra obtained from human skin. The spectral curves were produced by scanning the excitation monochromator from 240 nm to within 20 nm of the position of the emission monochromator (e.g., the first curve is produced by scanning the excitation monochromator from 240 nm to 300 nm with the emission monochromator set at 320 nm, the second by scanning the excitation from 240 nm to 320 nm with the emission set at 340 nm, and so on). The principal components of the spectra are indicated below the set of curves and correspond to (i) tryptophan, (ii) pepsin digestible collagen cross-links, (iii) collagenase digestible collagen cross-links, and (iv) elastin cross-links. Journal of Investigative Dermatology Symposium Proceedings 2002 7, 64-75DOI: (10.1046/j.1523-1747.2002.19635.x) Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions

Figure 8 Schematic diagram of an ATR crystal. The tip of the crystal (approximately 2 mm in diameter) is brought into contact with the skin sample. Light from an infrared source bounces twice at the walls of the conical tip of the probe. At each bounce an evanescent field extends beyond the crystal surface into the sample at a distance of approximately a quarter to a half the wavelength of the incident light. The reflected light creates an interference pattern with part of the illumination light in a similar configuration to Figure 2. Journal of Investigative Dermatology Symposium Proceedings 2002 7, 64-75DOI: (10.1046/j.1523-1747.2002.19635.x) Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions

Figure 9 Typical ATR-FTIR spectrum obtained from human skin. The ATR probe was placed in contact with the skin site of interest and the FTIR spectrum was acquired. The principal components contributing to the spectrum are (i) water, (ii) lipids, (iii) proteins. Region (iv) contains information from proteins, lipids, DNA, and water and is termed the “fingerprint spectral region”. Journal of Investigative Dermatology Symposium Proceedings 2002 7, 64-75DOI: (10.1046/j.1523-1747.2002.19635.x) Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions

Figure 10 Images obtained under polarized light illumination. (a) The analyzing polarizing filter was parallel to the illumination polarization filter; (b) the analyzing polarizing filter was positioned perpendicular to the illumination polarizing filter. In the images shown (a) the surface features of the skin become selectively enhanced and (b) the surface features of the skin are eliminated making possible the documentation of subsurface features such as erythema and pigmentation. Journal of Investigative Dermatology Symposium Proceedings 2002 7, 64-75DOI: (10.1046/j.1523-1747.2002.19635.x) Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions

Figure 11 Images obtained from the skin of an acne subject. (a) A fluorescence image excited with blue light (400 nm±10 nm). (b) Reflectance image with polarized illumination and perpendicular orientation of the analyzing polarizer – the surface features of the skin are absent from the image. (c) Reflectance image under camera flash illumination –both the surface of the skin and some subsurface features are seen. In image (a) the fluorescence emission of open comedones (noninflammatory lesions) is clearly delineated. In image (b) the inflammatory lesions are selectively shown in the absence of surface glare –the marks correspond to the locations of the noninflammatory lesions. In image (c) the marks show the noninflammatory lesions and the enhancement of the inflammatory lesions of image (b) is partially lost, making it difficult to count lesions or the extent of the inflammatory lesions. Journal of Investigative Dermatology Symposium Proceedings 2002 7, 64-75DOI: (10.1046/j.1523-1747.2002.19635.x) Copyright © 2002 The Society for Investigative Dermatology, Inc Terms and Conditions