Inverse problem of EIT using spectral constraints Emma Malone 1, Gustavo Santos 1, David Holder 1, Simon Arridge 2 1 Department of Medical Physics and.

Slides:



Advertisements
Similar presentations
Bayesian Belief Propagation
Advertisements

Fast & Furious: a potential wavefront reconstructor for extreme adaptive optics at ELTs Visa Korkiakoski and Christoph U. Keller Leiden Observatory Niek.
Slides from: Doug Gray, David Poole
Lect.3 Modeling in The Time Domain Basil Hamed
Computational Modeling for Engineering MECN 6040
1 Low-Dose Dual-Energy CT for PET Attenuation Correction with Statistical Sinogram Restoration Joonki Noh, Jeffrey A. Fessler EECS Department, The University.
Image Reconstruction and Image Priors Vadim Soloviev, Josias Elisee, Tim Rudge, Simon Arridge Munich April 24, 2009 TexPoint fonts used in EMF. Read the.
Inversion of coupled groundwater flow and heat transfer M. Bücker 1, V.Rath 2 & A. Wolf 1 1 Scientific Computing, 2 Applied Geophysics Bommerholz ,
Numerical Method for Computing Ground States of Spin-1 Bose-Einstein Condensates Fong Yin Lim Department of Mathematics and Center for Computational Science.
Multi-Task Compressive Sensing with Dirichlet Process Priors Yuting Qi 1, Dehong Liu 1, David Dunson 2, and Lawrence Carin 1 1 Department of Electrical.
3D Inversion of the Magnetic Field from Polarimetry Data of Magnetically Sensitive Coronal Ions M. Kramar, B. Inhester Max-Planck Institute for Solar System.
Presenter: Yufan Liu November 17th,
Inversion of Z-Axis Tipper Electromagnetic (Z-TEM)‏ Data The UBC Geophysical Inversion Facility Elliot Holtham and Douglas Oldenburg.
Effective gradient-free methods for inverse problems Jyri Leskinen FiDiPro DESIGN project.
High Frequency Ultrasonic Characterization of Carrot Tissue Christopher Vick Advisor: Dr. Navalgund Rao Center for Imaging Science Rochester Institute.
1 Adaptive error estimation of the Trefftz method for solving the Cauchy problem Presenter: C.-T. Chen Co-author: K.-H. Chen, J.-F. Lee & J.-T. Chen BEM/MRM.
Nanoparticle Polarizability Determination Using Coherent Confocal Microscopy Brynmor J. Davis and P. Scott Carney University of Illinois at Urbana-Champaign.
Preprocessing II: Between Subjects John Ashburner Wellcome Trust Centre for Neuroimaging, 12 Queen Square, London, UK.
Numerical methods for PDEs PDEs are mathematical models for –Physical Phenomena Heat transfer Wave motion.
Research Methods Ass. Professor, Community Medicine, Community Medicine Dept, College of Medicine.
Hanne Tiesler – 1 Identification of Material Parameters for Thermal Ablation Hanne Tiesler University of Bremen, Germany DFG SPP 1253.
IMAGING THE MIND Direct methods –Electrical activity (EEG, MEG) –Metabolic activity (EROS) Indirect methods –Changes in regional Cerebral Blood Flow (rCBF)
1/9/2007Bilkent University, Physics Department1 Supercontinuum Light Generation in Nano- and Micro-Structured Fibers Mustafa Yorulmaz Bilkent University.
Numerical modeling of the electromagnetic coupling effects for phase error correction in EIT borehole measurement Y Zhao1, E Zimmermann1, J A Huisman2,
Saratov State University ______________________________________________ Department of Optics & Biophotonics __________________________________________________.
On Estimation of Surface Soil Moisture from SAR Jiancheng Shi Institute for Computational Earth System Science University of California, Santa Barbara.
Computational Model of a Capillary: The effect of geometry on hemoglobin measurements Eugene Joh Medical Biophysics 6-Week Project Supervisor: Dr. Dan.
Lotte Ramekers. Research questions Introduction Models Methods Experiments and results Conclusions Questions.
IE 585 Introduction to Neural Networks. 2 Modeling Continuum Unarticulated Wisdom Articulated Qualitative Models Theoretic (First Principles) Models Empirical.
DTU Medical Visionday May 27, 2009 Generative models for automated brain MRI segmentation Koen Van Leemput Athinoula A. Martinos Center for Biomedical.
Improving the object depth localization in fluorescence diffuse optical tomography in an axial outward imaging geometry using a geometric sensitivity difference.
MA5251: Spectral Methods & Applications
2 2  Background  Vision in Human Brain  Efficient Coding Theory  Motivation  Natural Pictures  Methodology  Statistical Characteristics  Models.
Federal Department of Home Affairs FDHA Federal Office of Meteorology and Climatology MeteoSwiss High-resolution data assimilation in COSMO: Status and.
Stochastic Linear Programming by Series of Monte-Carlo Estimators Leonidas SAKALAUSKAS Institute of Mathematics&Informatics Vilnius, Lithuania
MAGNETIC NANOASSEMBLIES in MEDICINE
BioE153:Imaging As An Inverse Problem Grant T. Gullberg
Xianwu Ling Russell Keanini Harish Cherukuri Department of Mechanical Engineering University of North Carolina at Charlotte Presented at the 2003 IPES.
Lecture I Sensors.
Ovijit Chaudhuri PhD candidate Department of Bioengineering,
Akram Bitar and Larry Manevitz Department of Computer Science
FMRI – Week 4 – Contrast Scott Huettel, Duke University MR Contrast FMRI Graduate Course (NBIO 381, PSY 362) Dr. Scott Huettel, Course Director.
1 Markov random field: A brief introduction (2) Tzu-Cheng Jen Institute of Electronics, NCTU
HEAT TRANSFER FINITE ELEMENT FORMULATION
Research Methods Ass. Professor, Community Medicine, Community Medicine Dept, College of Medicine.
Introduction In positron emission tomography (PET), each line of response (LOR) has a different sensitivity due to the scanner's geometry and detector.
CardioInspect Diagnostic and Monitoring Systems
Impact of Axial Compression for the mMR Simultaneous PET-MR Scanner Martin A Belzunce, Jim O’Doherty and Andrew J Reader King's College London, Division.
Developing outcome prediction models for acute intracerebral hemorrhage patients: evaluation of a Support Vector Machine based method A. Jakab 1, L. Lánczi.
Neural Networks. Background - Neural Networks can be : Biological - Biological models Artificial - Artificial models - Desire to produce artificial systems.
The current density at each interfacial layer. The forward voltage is continuous at every point inside the body. A Layered Model for Breasts in Electrical.
Lyα Forest Simulation and BAO Detection Lin Qiufan Apr.2 nd, 2015.
Deep Learning Overview Sources: workshop-tutorial-final.pdf
Lecture Objectives: Accuracy of the Modeling Software.
Machine Learning Artificial Neural Networks MPλ ∀ Stergiou Theodoros 1.
Modelling & Simulation of Semiconductor Devices Lecture 1 & 2 Introduction to Modelling & Simulation.
Microstructure Imaging Sequence Simulation Toolbox
“ROSATOM” STATE CORPORATION ROSATOM
T. E. Dyhoum1, D. Lesnic 1 and R. G. Aykroyd 2
Excitation based cone-beam X-ray luminescence tomography of nanophosphors with different concentrations Peng Gao*, Huangsheng Pu*, Junyan Rong, Wenli Zhang,
Assessing Disclosure Risk in Microdata
Restricted Boltzmann Machines for Classification
Tianshuai Liu1, Junyan Rong1, Peng Gao1, Hongbing Lu1
Sahar Sargheini, Alberto Paganini, Ralf Hiptmair, Christian Hafner
Introduction to Biosensors
Failure Determination in Embedded Biomaterials
Prepared by: Mahmoud Rafeek Al-Farra
LAB MEETING Speaker : Cheolsun Kim
Akram Bitar and Larry Manevitz Department of Computer Science
Presentation transcript:

Inverse problem of EIT using spectral constraints Emma Malone 1, Gustavo Santos 1, David Holder 1, Simon Arridge 2 1 Department of Medical Physics and Bioengineering, University College London, UK 2 Department of Computer Science, University College London, UK

Introduction: EIT of acute stroke Ischaemic Haemorrhagic Stroke is the leading cause of disability and third cause of mortality in industrialized nations. Clot-busting drugs can improve the outcome of ischaemic stroke, but they need to be administered FAST !

Simple FD Weighted FD Jun et al (2009), Phys. Meas., 30(10), Nonlinear absolute Introduction: Multifrequency EIT background perturbation High sensitivity to errors Very limited application Limited application

Method: Fraction model The following assumptions are made: 1.the domain is composed of a known number T of tissues with distinct conductivity, 2.the conductivity of each tissue is known for all measurement frequencies, 3.the conductivity of the nth element is given by the linear combination of the conductivities of the component tissues where and.

x ω background perturbation x x ω Method: Fraction model ? ConductivityTissue spectraFraction values

Method: Fraction reconstruction Conductivity Fractions Markov Random field regularization:

Method: Fraction reconstruction Numerical validation Fractions Model Minimize… …subject to Step 1. Gradient projection Step 2. Damped Gauss-Newton repeat

Results: Use of difference data Phantom FractionsAbsolute Conductivities Difference data Absolute data

Results: Use of all multifrequency data Phantom Fractions All frequencies Single frequency WFD Conductivities

Results: Use of nonlinear method Model Fractions WFD Conductivities Nonlinear method Linear method

Discussion Advantages: Simultaneous and direct use of all multifrequency data Nonlinear reconstruction method Use of difference data Disadvantage: Requires accurate knowledge of tissue spectra. Temperature? Flow rate? Cell count?

Hiltunen P, Prince S J D, & Arridge S (2009). A combined reconstruction-classification method for diffuse optical tomography. Physics in medicine and biology, 54(21), 6457–76. Future work Hidden variable Tissue properties 1.Reconstruction 2.Classification

Centre for Medical Imaging and Computing (CMIC) Electrical Impedance Tomography (EIT) Research Group Department of Medical Physics and Bioengineering, University College London Thank for your attention