Anne-Sophie MONTCUQUET 1,2, Lionel HERVE 1, Jean-Marc DINTEN 1, Jérôme I. MARS 2 1 LETI / LISA – CEA, Minatec, 17 rue des Martyrs, 38054 Grenoble Cedex.

Slides:



Advertisements
Similar presentations
Hyperspectral two-photon near- infrared cancer imaging at depth Nikolay S. Makarov, Jean Starkey, Mikhail Drobizhev, Aleksander Rebane, Montana State University,
Advertisements

Sergey Kucheryavski Raman spectroscopy Acquisition, preprocessing and analysis of spectra.
Image-Pro Premier Basic Training Course
Live Imaging and Other Capabilities of the Bioscience Imaging Facility (BIF)
Optical Coherence Tomography Zhongping Chen, Ph.D. Optical imaging in turbid media Coherence and interferometry Optical coherence.
Fluorescence Diffuse Optical Tomography (FDOT) Our group presented three-dimensional (3D) in vivo images of human breast cancer based on fluorescence diffuse.
Effects of Fluorescence Self Absorption of Algae in Sea Water Candy Barbaran Annie Becerra Mentors: Prof. Fred Moshary Dr. Alex Gilerson NYCRI C N p.
IFTSUV: an Imaging Fourier Transform Spectrometer in the UV Anne Millard, 3 rd year PhD student, directed by P. Lemaire and J.-C. Vial.
Set-up for Levy Flight of Photons in Resonant Atomic Vapor Danielle Citro (SUNY Oswego), Adailton Feliciano (UFPB), Martine Chevrollier (UFPB), Marcos.
LINE PARAMETERS OF WATER VAPOR IN THE NEAR- AND MID-INFRARED REGIONS DETERMINED USING TUNEABLE LASER SPECTROSCOPY Nofal IBRAHIM, Pascale CHELIN, Johannes.
SINGLE CHANNEL SPEECH MUSIC SEPARATION USING NONNEGATIVE MATRIXFACTORIZATION AND SPECTRAL MASKS Jain-De,Lee Emad M. GraisHakan Erdogan 17 th International.
© CEA Tous droits réservés. Toute reproduction totale ou partielle sur quelque support que ce soit ou utilisation du contenu de ce document est interdite.
SIAMOIS, kickoff meeting, Paris, may, SIAMOIS: optical test bench BOSS (Banc Optique SiamoiS) Pernelle Bernardi Observatoire de Paris-Meudon,
Lyes Lakhal Institut Polytechnique LaSalle Beauvais Rue Pierre WAGUET
Evaluating new therapies in GIST using in vivo molecular imaging Lori Rink, Ph.D Fox Chase Cancer Center.
Test of the proposed method Introduction CCD Controller CCD Illuminator gel Filter 585nm Assembling the phantom before its irradiation. The phantom, ready.
Optical Characterization of GaN-based Nanowires : From Nanometric Scale to Light Emitting Devices A-L. Bavencove*, E. Pougeoise, J. Garcia, P. Gilet, F.
Quantitative Chemical Analysis Seventh Edition Quantitative Chemical Analysis Seventh Edition Chapter 0 The Analytical Process Copyright © 2007 by W. H.
SPECTRO-TEMPORAL POST-SMOOTHING IN NMF BASED SINGLE-CHANNEL SOURCE SEPARATION Emad M. Grais and Hakan Erdogan Sabanci University, Istanbul, Turkey  Single-channel.
In Silico Simulation of a Translational Human Breast Cancer Model in Mice March 25 th, 2013 Mark Dawidek Department of Medical Biophysics.
Improving the object depth localization in fluorescence diffuse optical tomography in an axial outward imaging geometry using a geometric sensitivity difference.
Andrey V. Zamyatin Femtosecond Ultra-Broadband Light Sources 4119 Twilight Ridge, San Diego, CA 92130, USA Tel:: (858) Fax:: (858) :
TIME-RESOLVED OPTICAL SPECTROSCOPY OF HIGH-TEMPERATURE PLASMAS M.J. Sadowski  , K. Malinowski , E. Skladnik-Sadowska , M. Scholtz , A. Tsarenko ¤
One Specific Velocity Color Mapping of Flows with Complex Geometry Biomedical Engineering, Tambov State Technical University, Russia S.G.Proskurin, A.Yu.Potlov,
Single Photon Emission Computed Tomography
Michal Tepper Under the supervision of Prof. Israel Gannot.
© CEA Tous droits réservés. Toute reproduction totale ou partielle sur quelque support que ce soit ou utilisation du contenu de ce document est interdite.
Gregory ClarkeTechnological Plasmas Research Group Time resolved diagnostics for pulsed magnetron plasmas.
Nuclear Medicine: Tomographic Imaging – SPECT, SPECT-CT and PET-CT Katrina Cockburn Nuclear Medicine Physicist.
Remon Ibrahim Remon Ibrahim High Energy Group.  Introduction  Experimental Techniques  Results  Conclusions Content.
Non-negative Matrix Factor Deconvolution; Extracation of Multiple Sound Sources from Monophonic Inputs International Symposium on Independent Component.
Part No...., Module No....Lesson No
A new spectroscopic observatory in Créteil to measure atmospheric trace gases in solar occultation geometry C. Viatte, P. Chelin, M. Eremenko, C. Keim,
Acquisition time6 min1 min 12 s Collimator height25 mm (Anger)12 mm (HiSens) Detector1 layer, 1 pixel / hole3 layers, 1 pixel / hole3 layers, 4 pixels.
DESCRIPTION OF PIXIRAD  The PIXIRAD Imaging Counter is an INFN-Pisa Spin-off  It works in photon counting  Pulse discrimination with two thresholds.
Date of download: 5/31/2016 Copyright © 2016 SPIE. All rights reserved. Example of a time-variant filter F(t,ω) designed using Eq. (9) to compensate for.
Date of download: 6/3/2016 Copyright © 2016 SPIE. All rights reserved. Schematic setup of the DS-VHI system. Multicolor fluorescent planes within a tissue.
Date of download: 6/3/2016 Copyright © 2016 SPIE. All rights reserved. (a) Representative Raman spectrum of bone. Major Raman bands are labeled along with.
Laser source 690 nm Spectrometer Translation stage: anesthezia B&W camera NλNλ NxNx NyNy CCD camera NxNx Anne-Sophie MONTCUQUET 1,2, Lionel HERVE 1, Fabrice.
Date of download: 9/17/2016 Copyright © 2016 SPIE. All rights reserved. Experimental layout. (a) Schematic of phantom showing the cross-sectional and overhead.
Date of download: 9/18/2016 Copyright © 2016 SPIE. All rights reserved. Schematic of the simultaneous time- and wavelength resolved fluorescence spectroscopy.
Date of download: 9/18/2016 Copyright © 2016 SPIE. All rights reserved. Schematic diagram of the spectroscopy module attached to the endoscopy imaging.
Spectroscopy and its Application
P.E.T. Positron Emission Tomography
Optical Non-Invasive Approaches to Diagnosis of Skin Diseases
Modulation-frequency dependency of optical measurements in turbid media: Phantom and simulation studies E L Maclin1, J Kimnach1, K A Low1 , M Fabiani1,
Excitation based cone-beam X-ray luminescence tomography of nanophosphors with different concentrations Peng Gao*, Huangsheng Pu*, Junyan Rong, Wenli Zhang,
Transient Absorption (Courtesy of Kenneth Hanson, Florida University): The technique applied to molecular dynamics Source hn Sample Detector.
Optical Coherence Tomography
Tianshuai Liu1, Junyan Rong1, Peng Gao1, Hongbing Lu1
Experimental modeling of local laser hyperthermia using thermosensitive nanoparticles absorbing in NIR Grachev P.V., Romanishkin I.D., Pominova D.V., Burmistrov.
When time does not heal wounds: Optical imaging of diabetic wounds
OPTICAL MONITORING OF PHOTOSENSITIZER DIFFUSION INTO TISSUE
Optical Non-Invasive Approaches to Diagnosis of Skin Diseases
AN ALGORITHM FOR LOCALIZATION OF OPTICAL STRUCTURE DISTURBANCES IN BIOLOGICAL TISSUE USING TIME-RESOLVED DIFFUSE OPTICAL TOMOGRAPHY Potlov A.Yu, Frolov.
Nicolas Bézière, Vasilis Ntziachristos  Gastroenterology 
MFM setup. MFM setup. The excitation lasers are combined in a fiber through an acousto-optic tunable filter, collimated, reflected on a dichroic mirror.
Volume 56, Issue 2, Pages (August 2009)
Quantum Dots for Molecular Pathology
Fourier Transform Emission Spectroscopy of CoH and CoD
Solving an estimation problem
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 
Complex Nanophotonics
NEUROIMAGING TECHNIQUE USING TIME-RESOLVED DIFFUSE OPTICAL TOMOGRAPHY AND INHOMOGENEITY LOCALIZATION ALGORITHM Potlov A.Yu, Frolov S.V., Proskurin S.G.
Vysakh Vasudevan*, N. Sujatha
Spectral-Polarization Sensors for in vivo Oncology Imaging
Yukihiro Hama, Yoshinori Koyama, Yasuteru Urano, Peter L
Non-negative Matrix Factorization (NMF)
Sensing Very Weak Strains at the Single-Molecule Scale
Presentation transcript:

Anne-Sophie MONTCUQUET 1,2, Lionel HERVE 1, Jean-Marc DINTEN 1, Jérôme I. MARS 2 1 LETI / LISA – CEA, Minatec, 17 rue des Martyrs, Grenoble Cedex 9, France. 2 GIPSA-Lab / Dept Images – Signal, 961 Rue de la Houille Blanche, BP 46, Saint Martin d'Hères, France. Introduction Fluorescent imaging in diffusive media is an emerging imaging modality for medical applications: injected fluorescent markers (in multiplexing, several specific markers are used) bind specifically to targeted compounds, like carcinoma. The region of interest is illuminated with near infrared light and the emitted back fluorescence is analyzed to localize the fluorescence sources. For medical diagnostic application, thick media have to be investigated: as the fluorescence signal gets exponentially weak with the light travel distance, any disturbing signal - such as biological tissues autofluorescence - may be a limiting factor. To remove these unwanted contributions, or to separate different fluorescent markers, a spectroscopic approach and a blind source separation method are explored. We present in this poster a feasibility experiment on an optical phantom in which a marked tumor is simulated. We show how an NMF unmixing preprocessing eradicates the autofluorescence signal of the phantom and allows to get more accurate 3-D reconstructions of the specific marker by Fluorescence Diffuse Optical Tomography (FDOT). Fluorescent imaging Image CEA Non-negative Matrix Factorization Therapeutic window Formal statement NMF applied to spectroscopy Given a non-negative matrix, find non-negative matrices and such that: (P stands for the number of fluorescent sources to unmix) Challenge We want to unmix several fluorescence spectra: A spectroscopic approach is chosen. We do not have much information about the fluorescence spectra : A blind source separation method is required. Conclusion Algorithm Multiplicative update rules Update of A: 1. Initialization of matrices A (constant) and S (spectra models) with A 0 and S 0 > 0 2. Minimization of the cost function F  Update, in turn, of A and S Algorithm steps Fluorescent probes location Non-negative Matrix Factorization: a blind sources separation method applied to optical fluorescence spectroscopy and multiplexing The use of red light limits the biological tissues absorption Injected fluorescent markers bind specifically to a given molecule Experimental set-up Update of S: The fluorescence signal is collected along a line of N x detectors by a spectrometer coupled with a CCD camera: a N x x N λ acquisition is measured. A translation stage, covering N y steps, is then used to get a scanning of the whole object. Feasibility experimentResults (1/2) Autofluorescence (PPIX) ICG-LNP Results (2/2) NMF decomposition gives two distinct fluorescence spectra. An original regularized NMF algorithm is used.. Experiments were performed ex vivo on optical phantoms to assess the capacity of NMF to unmix overlapping specific fluorescence and autofluorescence spectra.. The NMF algorithm is also suitable for in vivo experiments.. Spectrally resolved acquisitions combined to NMF processing successfully separate different fluorescent markers or filter different fluorescence contributions of interest from measurements impaired by autofluorescence.. NMF preprocessing improves FDOT reconstructions of specific fluorescent markers distributions by removing the disturbing fluorescence signals Intensity data Forward model: finite volume method *Andor technologies * * 690 nm