3/27/2012 WHY SPECT / CT? SPECT / CT Basic Principles. Advantages of SPECT. Advantages of CT. Dr John C. Dickson, Principal Physicist UCLH
|
|
- Oswald Burns
- 5 years ago
- Views:
Transcription
1 3/27/212 Advantages of SPECT SPECT / CT Basic Principles Dr John C. Dickson, Principal Physicist UCLH Institute of Nuclear Medicine, University College London Hospitals and University College London john.dickson@uclh.nhs.uk Advantages of CT WHY SPECT / CT? 1
2 3/27/212 Localisation Corrections: Attenuation Complementary Information SPECT / CT BY REGISTRATION 2
3 3/27/212 SPECT / CT by Registration SPECT / CT by Registration Acquire SPECT Acquire CT Overlay Data SIMPLE.. Match Patient Positioning Arms up or down? Sometimes not important Cushions, arm, and leg support Keep it as simple and reproducible as possible Breathing Protocol SPECT acquired over 3 minutes CT can be acquired less than 2 seconds Use end inspiration / end expiration / free breathing? Table top 3
4 3/27/212 Image Registration Image registration methodology Manually shift data Difficult and prone to errors Computer algorithm to shift data Manually define three or more anatomical landmarks on both data sets Fully automatic method using measures of similarity between data All data or a subsection of data Translate Rotate Translate Rotate Warp SPECT / CT by Registration Works best for simple structures e.g brain More difficult for Limbs Extremely difficult for moving or deformable structures e.g. lung, breast Proven successful for cardiac perfusion and CT coronary angiography Technical, co-ordination and workflow challenges Patient positioning critical 4
5 3/27/212 Transition to SPECT / CT The SPECT / CT System CT SPECT SPECT / CT Systems SPECT BASICS 5
6 3/27/212 SPECT SPECT Adapted from Sharp, Gemmell, Murray Filtered Back Projection (FBP) BP original NO CHANGE estimate patient original projections update (x ratio) Back Projection Filtered Back Projection ML-EM reconstruction Courtesy B. Hutton (UCL) estimated projections FP current estimate 6
7 3/27/212 Iterative Reconstruction Single Photon Emission Tomography ML-EM Computationally very expensive (Many projections) OS ML-EM (OSEM) Groups projection data into ordered sequence of subsets E.g. Subset size of 4: 1, 17,33,49;... Is an order of magnitude quicker than ML-EM Defined by number of iterations and subsets e.g. 2 iterations of 2 subsets (subset size of 6 for 12 projections) is equivalent to 4 iterations of ML-EM Comparing CT with SPECT CT BASICS 7
8 3/27/212 CT Scanner Comparing CT with SPECT CT Radiation can be turned on/off as required Radiation in required direction only Large number of photons Projections: Sum of attenuation Accurate Quantification SPECT Radiation present until decayed / excreted Isotopic radiation (most not detected) Fewer photons (~1 5 ) Projections: Sum of attenuated emissions Difficult to quantitate CT Reconstruction FBP Iterative (now) idose (Philips) IRIS (Siemens) ASIR (GE) Scanning Mode Axial, Helical, Cine Rotation time Slice Thickness Table Speed Helical Pitch Tube Current (Modulation) Dose Information Imaging Extent Shaping Filter kv Field of View (Zoom) Field Position Recon Filter 8
9 3/27/212 CT Parameters Scanning Mode Helical: Continuous sweep down subject Axial: Step and shoot. Cine: Used for dynamic studies e.g. using contrast Table speed / Pitch (Helical only) Determines tightness of spiral Large pitch means more interpolation to determine slices Shaping Filter (aka Bow-tie filter) Used to control dose to extremities Centre of field of view has more attenuation than edges, so we shape the beam to give more flux through centre CT parameters kvp: Potential difference across CT tube Higher kvp produce more penetrating X-rays Higher kvp increases dose to patient Tube Current (ma) Intensity/Flux of photons High ma, more photons, better image High ma, more dose Modulating ma can: Increase ma for high attenuation slices e.g. Pelvis Increase ma for lateral views compared to AP views BOTH Also ECG Modulation for cardiac studies CT Parameters CT Parameters Field of View (DFOV) Gives zoom facility to allow e.g. 25cm field of view for brain studies Can move field of view Reconstruction filters Standard, Soft (Tissue), Bone Predefined sharp or smooth filters Don t name using type and cut-off like SPECT CTDIvol Gives estimate of dose per cm of patient scanned Defined on phantoms e.g. Body DLP (Dose Length Product) Product of CTDIvol and length of body scanned Dose effectiveness (%) Amount of dose which is useful to produce image 9
10 3/27/212 CT Parameters used in SPECT / CT SPECT / CT systems available Low dose CT (< 5 mas per slice) Attenuation Correction Limited anatomical mapping > 5mm slice thickness Mid dose CT (5-1 mas per slice) Improved Anatomical Mapping Simple diagnostic imaging > 2.5 mm slice thickness High dose CT (> 1 mas per slice) Diagnostic Imaging Contrast Thin slices Gated and dynamic acquisitions Inherent Registration SPECT / CT: LOCALISATION CT SPECT 1
11 3/27/212 Inherent Registration Known mechanical displacement Software tweaks Registered SPECT/CT Inherent Registration? System Related misregistration Poor alignment calibration x Bed Sag Issues - Misregistration Comparison of breath hold and tidal breathing 12 second Patient related misregistration Patient movement SPECT scan duration 2-4 minutes CT scan duration 2-1 minutes (GE Hawkeye) 1-4 seconds (Philips, Siemens) Breath hold CT, 12kVp, 5mA, 1ms pulse width,.8mgy 6 second Tidal breathing CT, 12kVp, 2.5mA, continuous CT, 1.2mGy Images courtesy of Radiological March 212: Associates BIR Londonof Sacramento 11
12 3/27/212 Software solution for Misregistration SPECT / CT: CORRECTIONS NB: Misregistration affects alignment and attenuation correction Iterative Reconstruction System matrix Estimate Activity Distribution Prior Knowledge Attenuation Resolution loss [Scatter] Forward Project Data to give Estimated Projections Compare Estimated and Measured Projections 1 pixel i 1 Difference? 1 No Yes Stop voxel j 12
13 3/27/212 Attenuation Correction System matrix: with attenuation.2.5 μ.9 Future? Scatter Correction Advantages of Scatter Correction Hutton BF et al: Phys Med Biol 56 (211) R85-R112 13
14 3/27/212 Thank you! 14
Philips SPECT/CT Systems
Philips SPECT/CT Systems Ling Shao, PhD Director, Imaging Physics & System Analysis Nuclear Medicine, Philips Healthcare June 14, 2008 *Presented SNM08 Categorical Seminar - Quantitative SPECT and PET
More informationGPU implementation for rapid iterative image reconstruction algorithm
GPU implementation for rapid iterative image reconstruction algorithm and its applications in nuclear medicine Jakub Pietrzak Krzysztof Kacperski Department of Medical Physics, Maria Skłodowska-Curie Memorial
More informationSpiral CT. Protocol Optimization & Quality Assurance. Ge Wang, Ph.D. Department of Radiology University of Iowa Iowa City, Iowa 52242, USA
Spiral CT Protocol Optimization & Quality Assurance Ge Wang, Ph.D. Department of Radiology University of Iowa Iowa City, Iowa 52242, USA Spiral CT Protocol Optimization & Quality Assurance Protocol optimization
More informationOptimization of CT Simulation Imaging. Ingrid Reiser Dept. of Radiology The University of Chicago
Optimization of CT Simulation Imaging Ingrid Reiser Dept. of Radiology The University of Chicago Optimization of CT imaging Goal: Achieve image quality that allows to perform the task at hand (diagnostic
More informationOptimisation of Toshiba Aquilion ONE Volume Imaging
Optimisation of Toshiba Aquilion ONE Volume Imaging Jane Edwards, RPRSG Royal Free London NHS Foundation Trust Dr Mufudzi Maviki, Plymouth Hospitals NHS Trust Background In 2011/12 Radiology at RFH was
More informationA closer look at CT scanning
Vet Times The website for the veterinary profession https://www.vettimes.co.uk A closer look at CT scanning Author : Charissa Lee, Natalie Webster Categories : General, Vets Date : April 3, 2017 A basic
More informationComputer-Tomography II: Image reconstruction and applications
Computer-Tomography II: Image reconstruction and applications Prof. Dr. U. Oelfke DKFZ Heidelberg Department of Medical Physics (E040) Im Neuenheimer Feld 280 69120 Heidelberg, Germany u.oelfke@dkfz.de
More informationCh. 4 Physical Principles of CT
Ch. 4 Physical Principles of CT CLRS 408: Intro to CT Department of Radiation Sciences Review: Why CT? Solution for radiography/tomography limitations Superimposition of structures Distinguishing between
More informationCT NOISE POWER SPECTRUM FOR FILTERED BACKPROJECTION AND ITERATIVE RECONSTRUCTION
CT NOISE POWER SPECTRUM FOR FILTERED BACKPROJECTION AND ITERATIVE RECONSTRUCTION Frank Dong, PhD, DABR Diagnostic Physicist, Imaging Institute Cleveland Clinic Foundation and Associate Professor of Radiology
More informationTechnical aspects of SPECT and SPECT-CT. John Buscombe
Technical aspects of SPECT and SPECT-CT John Buscombe What does the clinician need to know? For SPECT What factors affect SPECT How those factors should be sought Looking for artefacts For SPECT-CT Issues
More informationSpiral ASSR Std p = 1.0. Spiral EPBP Std. 256 slices (0/300) Kachelrieß et al., Med. Phys. 31(6): , 2004
Spiral ASSR Std p = 1.0 Spiral EPBP Std p = 1.0 Kachelrieß et al., Med. Phys. 31(6): 1623-1641, 2004 256 slices (0/300) Advantages of Cone-Beam Spiral CT Image quality nearly independent of pitch Increase
More informationCT Basics Principles of Spiral CT Dose. Always Thinking Ahead.
1 CT Basics Principles of Spiral CT Dose 2 Who invented CT? 1963 - Alan Cormack developed a mathematical method of reconstructing images from x-ray projections Sir Godfrey Hounsfield worked for the Central
More informationAIDR 3D Iterative Reconstruction:
Iterative Reconstruction: Integrated, Automated and Adaptive Dose Reduction Erin Angel, PhD Manager, Clinical Sciences, CT Canon Medical Systems USA Iterative Reconstruction 1 Since the introduction of
More informationWorkshop on Quantitative SPECT and PET Brain Studies January, 2013 PUCRS, Porto Alegre, Brasil Corrections in SPECT and PET
Workshop on Quantitative SPECT and PET Brain Studies 14-16 January, 2013 PUCRS, Porto Alegre, Brasil Corrections in SPECT and PET Físico João Alfredo Borges, Me. Corrections in SPECT and PET SPECT and
More informationMetal Artifact Reduction CT Techniques. Tobias Dietrich University Hospital Balgrist University of Zurich Switzerland
Metal Artifact Reduction CT Techniques R S S S Tobias Dietrich University Hospital Balgrist University of Zurich Switzerland N. 1 v o 4 1 0 2. Postoperative CT Metal Implants CT is accurate for assessment
More informationShadow casting. What is the problem? Cone Beam Computed Tomography THE OBJECTIVES OF DIAGNOSTIC IMAGING IDEAL DIAGNOSTIC IMAGING STUDY LIMITATIONS
Cone Beam Computed Tomography THE OBJECTIVES OF DIAGNOSTIC IMAGING Reveal pathology Reveal the anatomic truth Steven R. Singer, DDS srs2@columbia.edu IDEAL DIAGNOSTIC IMAGING STUDY Provides desired diagnostic
More informationIntroduction to Biomedical Imaging
Alejandro Frangi, PhD Computational Imaging Lab Department of Information & Communication Technology Pompeu Fabra University www.cilab.upf.edu X-ray Projection Imaging Computed Tomography Digital X-ray
More informationTomographic Reconstruction
Tomographic Reconstruction 3D Image Processing Torsten Möller Reading Gonzales + Woods, Chapter 5.11 2 Overview Physics History Reconstruction basic idea Radon transform Fourier-Slice theorem (Parallel-beam)
More informationMulti-slice CT Image Reconstruction Jiang Hsieh, Ph.D.
Multi-slice CT Image Reconstruction Jiang Hsieh, Ph.D. Applied Science Laboratory, GE Healthcare Technologies 1 Image Generation Reconstruction of images from projections. textbook reconstruction advanced
More information8/2/2016. Measures the degradation/distortion of the acquired image (relative to an ideal image) using a quantitative figure-of-merit
Ke Li Assistant Professor Department of Medical Physics and Department of Radiology School of Medicine and Public Health, University of Wisconsin-Madison This work is partially supported by an NIH Grant
More informationBME I5000: Biomedical Imaging
1 Lucas Parra, CCNY BME I5000: Biomedical Imaging Lecture 4 Computed Tomography Lucas C. Parra, parra@ccny.cuny.edu some slides inspired by lecture notes of Andreas H. Hilscher at Columbia University.
More informationImage Acquisition Systems
Image Acquisition Systems Goals and Terminology Conventional Radiography Axial Tomography Computer Axial Tomography (CAT) Magnetic Resonance Imaging (MRI) PET, SPECT Ultrasound Microscopy Imaging ITCS
More informationRadiology. Marta Anguiano Millán. Departamento de Física Atómica, Molecular y Nuclear Facultad de Ciencias. Universidad de Granada
Departamento de Física Atómica, Molecular y Nuclear Facultad de Ciencias. Universidad de Granada Overview Introduction Overview Introduction Tecniques of imaging in Overview Introduction Tecniques of imaging
More informationLimits of Dose Reduction in CT: How low is too low? Acknowledgement. Disclosures 8/2/2012
8/2/22 Limits of Dose Reduction in CT: How low is too low? Ehsan Samei Duke University Acknowledgement Disclosures Research grant: NIH Research grant: DHS Research grant: RSNA, QIBA Research grant: General
More informationCardiac Dual Energy CT: Technique
RSNA 2013, VSCA51-01, Chicago, Dec. 5, 2013 Cardiac Radiology Series Cardiac Dual Energy CT: Technique Willi A. Kalender, Ph.D. Institute of Medical Physics University of Erlangen www.imp.uni-erlangen.de
More informationIntroduction to Positron Emission Tomography
Planar and SPECT Cameras Summary Introduction to Positron Emission Tomography, Ph.D. Nuclear Medicine Basic Science Lectures srbowen@uw.edu System components: Collimator Detector Electronics Collimator
More informationTomoTherapy Related Projects. An image guidance alternative on Tomo Low dose MVCT reconstruction Patient Quality Assurance using Sinogram
TomoTherapy Related Projects An image guidance alternative on Tomo Low dose MVCT reconstruction Patient Quality Assurance using Sinogram Development of A Novel Image Guidance Alternative for Patient Localization
More informationDiagnostic imaging techniques. Krasznai Zoltán. University of Debrecen Medical and Health Science Centre Department of Biophysics and Cell Biology
Diagnostic imaging techniques Krasznai Zoltán University of Debrecen Medical and Health Science Centre Department of Biophysics and Cell Biology 1. Computer tomography (CT) 2. Gamma camera 3. Single Photon
More informationRADIOLOGY AND DIAGNOSTIC IMAGING
Day 2 part 2 RADIOLOGY AND DIAGNOSTIC IMAGING Dr hab. Zbigniew Serafin, MD, PhD serafin@cm.umk.pl 2 3 4 5 CT technique CT technique 6 CT system Kanal K: RSNA/AAPM web module: CT Systems & CT Image Quality
More informationFits you like no other
Fits you like no other BrightView X and XCT specifications The new BrightView X system is a fully featured variableangle camera that is field-upgradeable to BrightView XCT without any increase in room
More informationCorso di laurea in Fisica A.A Fisica Medica 4 TC
Corso di laurea in Fisica A.A. 2007-2008 Fisica Medica 4 TC Computed Tomography Principles 1. Projection measurement 2. Scanner systems 3. Scanning modes Basic Tomographic Principle The internal structure
More informationML reconstruction for CT
ML reconstruction for CT derivation of MLTR rigid motion correction resolution modeling polychromatic ML model dual energy ML model Bruno De Man, Katrien Van Slambrouck, Maarten Depypere, Frederik Maes,
More informationSPECT reconstruction
Regional Training Workshop Advanced Image Processing of SPECT Studies Tygerberg Hospital, 19-23 April 2004 SPECT reconstruction Martin Šámal Charles University Prague, Czech Republic samal@cesnet.cz Tomography
More informationValidation of GEANT4 for Accurate Modeling of 111 In SPECT Acquisition
Validation of GEANT4 for Accurate Modeling of 111 In SPECT Acquisition Bernd Schweizer, Andreas Goedicke Philips Technology Research Laboratories, Aachen, Germany bernd.schweizer@philips.com Abstract.
More informationSPECT QA and QC. Bruce McBride St. Vincent s Hospital Sydney.
SPECT QA and QC Bruce McBride St. Vincent s Hospital Sydney. SPECT QA and QC What is needed? Why? How often? Who says? QA and QC in Nuclear Medicine QA - collective term for all the efforts made to produce
More informationThe Near Future in Cardiac CT Image Reconstruction
SCCT 2010 The Near Future in Cardiac CT Image Reconstruction Marc Kachelrieß Institute of Medical Physics (IMP) Friedrich-Alexander Alexander-University Erlangen-Nürnberg rnberg www.imp.uni-erlangen.de
More informationAcknowledgments and financial disclosure
AAPM 2012 Annual Meeting Digital breast tomosynthesis: basic understanding of physics principles James T. Dobbins III, Ph.D., FAAPM Director, Medical Physics Graduate Program Ravin Advanced Imaging Laboratories
More informationEnhancement Image Quality of CT Using Single Slice Spiral Technique
Enhancement Image Quality of CT Using Single Slice Spiral Technique Doaa. N. Al Sheack 1 and Dr.Mohammed H. Ali Al Hayani 2 1 2 Electronic and Communications Engineering Department College of Engineering,
More informationMEDICAL EQUIPMENT: COMPUTED TOMOGRAPHY. Prof. Yasser Mostafa Kadah
MEDICAL EQUIPMENT: COMPUTED TOMOGRAPHY Prof. Yasser Mostafa Kadah www.k-space.org Recommended Textbook X-Ray Computed Tomography in Biomedical Engineering, by Robert Cierniak, Springer, 211 Computed Tomography
More informationContrast Enhancement with Dual Energy CT for the Assessment of Atherosclerosis
Contrast Enhancement with Dual Energy CT for the Assessment of Atherosclerosis Stefan C. Saur 1, Hatem Alkadhi 2, Luca Regazzoni 1, Simon Eugster 1, Gábor Székely 1, Philippe Cattin 1,3 1 Computer Vision
More informationMedical Image Analysis
Computer assisted Image Analysis VT04 29 april 2004 Medical Image Analysis Lecture 10 (part 1) Xavier Tizon Medical Image Processing Medical imaging modalities XRay,, CT Ultrasound MRI PET, SPECT Generic
More information11/18/ CPT Preauthorization Groupings Effective January 1, Computerized Tomography (CT) Abdomen 6. CPT Description SEGR CT01
Computerized Tomography (CT) 6 & 101 5 Upper Extremity 11 Lower Extremity 12 Head 3 Orbit 1 Sinus 2 Neck 4 7 Cervical Spine 8 Thoracic Spine 9 Lumbar Spine 10 Colon 13 CPT Description SEGR 74150 74160
More informationDeviceless respiratory motion correction in PET imaging exploring the potential of novel data driven strategies
g Deviceless respiratory motion correction in PET imaging exploring the potential of novel data driven strategies Presented by Adam Kesner, Ph.D., DABR Assistant Professor, Division of Radiological Sciences,
More informationCT: Physics Principles & Equipment Design
CT: Physics Principles & Equipment Design James Kofler, Ph.D Radiology Mayo Clinic Rochester, MN June 27, 2012 Disclosures Nothing to disclose Learning Objectives Understand fundamental concepts of - CT
More informationIterative Reconstructions: The Impact on Dose and Image Quality
Shane Foley: IPR, Chicago 2016 Iterative Reconstructions: The Impact on Dose and Image Quality Shane Foley, PhD Radiography and Diagnostic Imaging School of Medicine University College Dublin. Radagrafaíocht
More informationDigital Image Processing
Digital Image Processing SPECIAL TOPICS CT IMAGES Hamid R. Rabiee Fall 2015 What is an image? 2 Are images only about visual concepts? We ve already seen that there are other kinds of image. In this lecture
More informationFits you like no other
Fits you like no other Philips BrightView X and XCT specifications The new BrightView X system is a fully featured variableangle camera that is field-upgradeable to BrightView XCT without any increase
More informationRespiratory Motion Estimation using a 3D Diaphragm Model
Respiratory Motion Estimation using a 3D Diaphragm Model Marco Bögel 1,2, Christian Riess 1,2, Andreas Maier 1, Joachim Hornegger 1, Rebecca Fahrig 2 1 Pattern Recognition Lab, FAU Erlangen-Nürnberg 2
More informationAnnexure XII SPECIFICATIONS FOR A NEW STATE OF ART 16 SLICE ALL PURPOSE C. T. SCANNER
Annexure XII SPECIFICATIONS FOR A NEW STATE OF ART 16 SLICE ALL PURPOSE C. T. SCANNER A) Scanner Design X-Ray generator and tube: 1. Scanner: Whole body spiral CT scanner (16 slices) of latest technology.
More informationConflicts of Interest Nuclear Medicine and PET physics reviewer for the ACR Accreditation program
James R Halama, PhD Loyola University Medical Center Conflicts of Interest Nuclear Medicine and PET physics reviewer for the ACR Accreditation program Learning Objectives 1. Be familiar with recommendations
More informationCT issues in PET / CT scanning. ImPACT technology update no. 4
abc David Platten Introduction ImPACT technology update no. 4 ImPACT October 2004 Since its introduction in the 1970s, X-ray computed tomography (CT) scanning has become a widespread three-dimensional
More information1. Deployment of a framework for drawing a correspondence between simple figure of merits (FOM) and quantitative imaging performance in CT.
Progress report: Development of assessment and predictive metrics for quantitative imaging in chest CT Subaward No: HHSN6801000050C (4a) PI: Ehsan Samei Reporting Period: month 1-18 Deliverables: 1. Deployment
More informationAdvanced Scatter Correction for Quantitative Cardiac SPECT
Advanced Scatter Correction for Quantitative Cardiac SPECT Frederik J. Beekman PhD Molecular Image Science Laboratory University Medical Center Utrecht The Netherlands Outline What is scatter? Scatter
More information4DM Packages. 4DM Packages & License Types. Information to help you order the appropriate licenses for your site.
4DM Packages 4DM Packages & License Types. Information to help you order the appropriate licenses for your site. Nuclear Cardiac Quantification, Review, and Reporting Select Your 4DM Package and corresponding
More informationReview of PET Physics. Timothy Turkington, Ph.D. Radiology and Medical Physics Duke University Durham, North Carolina, USA
Review of PET Physics Timothy Turkington, Ph.D. Radiology and Medical Physics Duke University Durham, North Carolina, USA Chart of Nuclides Z (protons) N (number of neutrons) Nuclear Data Evaluation Lab.
More informationReconstruction from Projections
Reconstruction from Projections M.C. Villa Uriol Computational Imaging Lab email: cruz.villa@upf.edu web: http://www.cilab.upf.edu Based on SPECT reconstruction Martin Šámal Charles University Prague,
More informationA Comparison of the Uniformity Requirements for SPECT Image Reconstruction Using FBP and OSEM Techniques
IMAGING A Comparison of the Uniformity Requirements for SPECT Image Reconstruction Using FBP and OSEM Techniques Lai K. Leong, Randall L. Kruger, and Michael K. O Connor Section of Nuclear Medicine, Department
More informationDUAL-ENERGY CT IN PROTON THERAPY
10/31/17 DUAL-ENERGY CT IN PROTON THERAPY Isabel Almeida, MAASTRO Clinic 7th NCS Lustrum Symposium 1 10/31/17 http://zonptc.bouwwebcam.nl https://www.youtube.com/watch?v=3vvvf5bqn7g Range uncertainties
More informationImplementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system
Implementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system 3 rd October 2008 11 th Topical Seminar on Innovative Particle and Radiation
More information8/7/2017. Disclosures. MECT Systems Overview and Quantitative Opportunities. Overview. Computed Tomography (CT) CT Numbers. Polyenergetic Acquisition
Quantitative Multi-Energy Computed Tomography: Imaging and Therapy Advancements Disclosures MECT Systems Overview and Quantitative Opportunities The speaker receives research funding from GE Healthcare
More informationInveon User Notes. Inveon Scanners and Inveon Acquisition Workplace 2.0
Inveon User Notes Inveon Scanners and Inveon Acquisition Workplace 2.0 Legal Notice 2014 by Siemens Medical Solutions USA, Inc. All rights reserved. Siemens reserves the right to modify the design and
More informationBrilliance CT Big Bore.
1 2 2 There are two methods of RCCT acquisition in widespread clinical use: cine axial and helical. In RCCT with cine axial acquisition, repeat CT images are taken each couch position while recording respiration.
More informationFundamentals of CT imaging
SECTION 1 Fundamentals of CT imaging I History In the early 1970s Sir Godfrey Hounsfield s research produced the first clinically useful CT scans. Original scanners took approximately 6 minutes to perform
More informationC a t p h a n / T h e P h a n t o m L a b o r a t o r y
C a t p h a n 5 0 0 / 6 0 0 T h e P h a n t o m L a b o r a t o r y C a t p h a n 5 0 0 / 6 0 0 Internationally recognized for measuring the maximum obtainable performance of axial, spiral and multi-slice
More informationBiomedical Imaging. Computed Tomography. Patrícia Figueiredo IST
Biomedical Imaging Computed Tomography Patrícia Figueiredo IST 2013-2014 Overview Basic principles X ray attenuation projection Slice selection and line projections Projection reconstruction Instrumentation
More informationAAPM Standard of Practice: CT Protocol Review Physicist
AAPM Standard of Practice: CT Protocol Review Physicist Dianna Cody, Ph.D., DABR, FAAPM U.T.M.D. Anderson Cancer Center September 11, 2014 2014 Texas Radiation Regulatory Conference Goals Understand purpose
More informationComputed Tomography. Principles, Design, Artifacts, and Recent Advances. Jiang Hsieh THIRD EDITION. SPIE PRESS Bellingham, Washington USA
Computed Tomography Principles, Design, Artifacts, and Recent Advances THIRD EDITION Jiang Hsieh SPIE PRESS Bellingham, Washington USA Table of Contents Preface Nomenclature and Abbreviations xi xv 1 Introduction
More informationSome reference material
Some reference material Physics reference book on medical imaging: A good one is The Essential Physics of Medical Imaging, 3 rd Ed. by Bushberg et al. ($170! new). However, there are several similar books
More informationAs fl exible as your care requires
As fl exible as your care requires Philips Ingenuity Flex 32 CT Built on Ingenuity The Philips Ingenuity Flex 32 helps you provide excellent care with outstanding flexibility, now and in the future. Built
More informationBackground 8/2/2011. Development of Breast Models for Use in Simulation of Breast Tomosynthesis and CT Breast Imaging. Stephen J.
Development of Breast Models for Use in Simulation of Breast Tomosynthesis and CT Breast Imaging Stephen J. Glick* J. Michael O Connor**, Clay Didier**, Mini Das*, * University of Massachusetts Medical
More informationPURE. ViSION Edition PET/CT. Patient Comfort Put First.
PURE ViSION Edition PET/CT Patient Comfort Put First. 2 System features that put patient comfort and safety first. Oncology patients deserve the highest levels of safety and comfort during scans. Our Celesteion
More informationImage Guidance and Beam Level Imaging in Digital Linacs
Image Guidance and Beam Level Imaging in Digital Linacs Ruijiang Li, Ph.D. Department of Radiation Oncology Stanford University School of Medicine 2014 AAPM Therapy Educational Course Disclosure Research
More informationDigital Scatter Removal in Mammography to enable Patient Dose Reduction
Digital Scatter Removal in Mammography to enable Patient Dose Reduction Mary Cocker Radiation Physics and Protection Oxford University Hospitals NHS Trust Chris Tromans, Mike Brady University of Oxford
More informationMotion Compensation from Short-Scan Data in Cardiac CT
Motion Compensation from Short-Scan Data in Cardiac CT Juliane Hahn 1,2, Thomas Allmendinger 1, Herbert Bruder 1, and Marc Kachelrieß 2 1 Siemens Healthcare GmbH, Forchheim, Germany 2 German Cancer Research
More informationMicro-CT Methodology Hasan Alsaid, PhD
Micro-CT Methodology Hasan Alsaid, PhD Preclinical & Translational Imaging LAS, PTS, GlaxoSmithKline 20 April 2015 Provide basic understanding of technical aspects of the micro-ct Statement: All procedures
More informationDisclosures 7/21/2014. AAPM 2014 Challenges and opportunities in assessment of image quality
7/2/24 AAPM 24 Challenges and opportunities in assessment of image quality Ehsan Samei Department of Radiology Duke University Medical Center Disclosures Research grant: NIH R EB838 Research grant: General
More informationMathematical methods and simulations tools useful in medical radiation physics
Mathematical methods and simulations tools useful in medical radiation physics Michael Ljungberg, professor Department of Medical Radiation Physics Lund University SE-221 85 Lund, Sweden Major topic 1:
More informationQIBA PET Amyloid BC March 11, Agenda
QIBA PET Amyloid BC March 11, 2016 - Agenda 1. QIBA Round 6 Funding a. Deadlines b. What projects can be funded, what cannot c. Discussion of projects Mechanical phantom and DRO Paul & John? Any Profile
More informationUvA-DARE (Digital Academic Repository) Motion compensation for 4D PET/CT Kruis, M.F. Link to publication
UvA-DARE (Digital Academic Repository) Motion compensation for 4D PET/CT Kruis, M.F. Link to publication Citation for published version (APA): Kruis, M. F. (2014). Motion compensation for 4D PET/CT General
More informationLower Dose with Confidence
Lower Dose with Confidence The Next Generation SCENARIA CT is Here. 64 or 128 Slice Capability The SCENARIA SE delivers lower dose technologies*, enhanced patient access, fast workflow speed and added
More informationThe protocols used to scan the musculoskeletal system are tailored to each patient and
Chapter 22. Musculoskeletal Protocols The protocols used to scan the musculoskeletal system are tailored to each patient and region being examined. The clinical indication for the examination will also
More informationSuitability of a new alignment correction method for industrial CT
Suitability of a new alignment correction method for industrial CT Matthias Elter 1, Nicole Maass 1, Peter Koch 2 1 Siemens AG, Healthcare Sector, Erlangen, Germany, e-mail: matthias.elter@siemens.com,
More informationHitachi Medical Systems America, Inc. Hitachi Medical Corporation
Advanced 128 Advanced 128 128 Slice Capability Enlarged 75cm Aperture Thin Gantry Profile 88cm Intelli IP Advanced, Iterative Reconstruction IntelliCenter Auto-Lateral Shifting Table, up to 16cm Range
More informationCT vs. VolumeScope: image quality and dose comparison
CT vs. VolumeScope: image quality and dose comparison V.N. Vasiliev *a, A.F. Gamaliy **b, M.Yu. Zaytsev b, K.V. Zaytseva ***b a Russian Sci. Center of Roentgenology & Radiology, 86, Profsoyuznaya, Moscow,
More informationAgenda : Lung Density Breakout Session
Agenda : Lung Density Breakout Session 1. : Mathew Fuld and Bernice Hoppel 2. Automatic Exposure Control (AEC) Evaluation : Sean Fain Round 4 Project 3. Dose reduction effects on emphysema metrics : Philip
More informationUSING cone-beam geometry with pinhole collimation,
IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 56, NO. 3, JUNE 2009 687 A Backprojection-Based Parameter Estimation Technique for Skew-Slit Collimation Jacob A. Piatt, Student Member, IEEE, and Gengsheng L.
More informationEstimating 3D Respiratory Motion from Orbiting Views
Estimating 3D Respiratory Motion from Orbiting Views Rongping Zeng, Jeffrey A. Fessler, James M. Balter The University of Michigan Oct. 2005 Funding provided by NIH Grant P01 CA59827 Motivation Free-breathing
More informationJames R Halama, PhD Loyola University Medical Center
James R Halama, PhD Loyola University Medical Center Conflicts of Interest Nuclear Medicine and PET physics reviewer for the ACR Accreditation program Learning Objectives Be familiar with the tests recommended
More informationA Radiometry Tolerant Method for Direct 3D/2D Registration of Computed Tomography Data to X-ray Images
A Radiometry Tolerant Method for Direct 3D/2D Registration of Computed Tomography Data to X-ray Images Transfer Function Independent Registration Boris Peter Selby 1, Georgios Sakas 2, Stefan Walter 1,
More informationNIH Public Access Author Manuscript Med Phys. Author manuscript; available in PMC 2009 March 13.
NIH Public Access Author Manuscript Published in final edited form as: Med Phys. 2008 February ; 35(2): 660 663. Prior image constrained compressed sensing (PICCS): A method to accurately reconstruct dynamic
More informationHidenobu Tachibana The Cancer Institute Hospital of JFCR, Radiology Dept. The Cancer Institute of JFCR, Physics Dept.
2-D D Dose-CT Mapping in Geant4 Hidenobu Tachibana The Cancer Institute Hospital of JFCR, Radiology Dept. The Cancer Institute of JFCR, Physics Dept. Table of Contents Background & Purpose Materials Methods
More informationComparison of the Imaging Performance of CT Scanners, Issue 11
Imaging Performance Assessment of CT Scanners Comparison of the Imaging Performance of CT Scanners, Issue 11 Comparison data is presented on the following scanners : Elscint Twin Flash IGE HiSpeed Advantage
More informationDUAL energy X-ray radiography [1] can be used to separate
IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 53, NO. 1, FEBRUARY 2006 133 A Scatter Correction Using Thickness Iteration in Dual-Energy Radiography S. K. Ahn, G. Cho, and H. Jeon Abstract In dual-energy
More informationRespiratory Motion Compensation for Simultaneous PET/MR Based on Strongly Undersampled Radial MR Data
Respiratory Motion Compensation for Simultaneous PET/MR Based on Strongly Undersampled Radial MR Data Christopher M Rank 1, Thorsten Heußer 1, Andreas Wetscherek 1, and Marc Kachelrieß 1 1 German Cancer
More informationFinancial disclosure. Onboard imaging modality for IGRT
Tetrahedron Beam Computed Tomography Based On Multi-Pixel X- Ray Source and Its Application in Image Guided Radiotherapy Tiezhi Zhang, Ph.D. Advanced X-ray imaging Lab Financial disclosure Patent royalty
More informationDesign and performance characteristics of a Cone Beam CT system for Leksell Gamma Knife Icon
Design and performance characteristics of a Cone Beam CT system for Leksell Gamma Knife Icon WHITE PAPER Introduction Introducing an image guidance system based on Cone Beam CT (CBCT) and a mask immobilization
More informationCT Protocol Clinical Graphics Move Forward 3D motion analysis service
CT Protocol Clinical Graphics Move Forward 3D motion analysis service Version 1.4 Description of contents This document describes the CT protocol of scans for Clinical Graphics Move Forward 3D Motion Simulation
More informationPhysical bases of X-ray diagnostics
Physical bases of X-ray diagnostics Dr. István Voszka Possibilities of X-ray production (X-ray is produced, when charged particles of high velocity are stopped) X-ray tube: Relatively low accelerating
More informationMotion artifact detection in four-dimensional computed tomography images
Motion artifact detection in four-dimensional computed tomography images G Bouilhol 1,, M Ayadi, R Pinho, S Rit 1, and D Sarrut 1, 1 University of Lyon, CREATIS; CNRS UMR 5; Inserm U144; INSA-Lyon; University
More informationCLASS HOURS: 4 CREDIT HOURS: 4 LABORATORY HOURS: 0
Revised 10/10 COURSE SYLLABUS TM 220 COMPUTED TOMOGRAPHY PHYSICS CLASS HOURS: 4 CREDIT HOURS: 4 LABORATORY HOURS: 0 CATALOG COURSE DESCRIPTION: This course is one of a three course set in whole body Computed
More information