Educational Objectives SPECT/CT: Basics, Quality Assurance, and Clinical Applications

Similar documents
SPECT/CT Basics, Technology Updates, Quality Assurance, and Applications

Conflicts of Interest Nuclear Medicine and PET physics reviewer for the ACR Accreditation program

James R Halama, PhD Loyola University Medical Center

Introduction to Emission Tomography

Introduction to Positron Emission Tomography

3/27/2012 WHY SPECT / CT? SPECT / CT Basic Principles. Advantages of SPECT. Advantages of CT. Dr John C. Dickson, Principal Physicist UCLH

Philips SPECT/CT Systems

Diagnostic imaging techniques. Krasznai Zoltán. University of Debrecen Medical and Health Science Centre Department of Biophysics and Cell Biology

Validation of GEANT4 for Accurate Modeling of 111 In SPECT Acquisition

Review of PET Physics. Timothy Turkington, Ph.D. Radiology and Medical Physics Duke University Durham, North Carolina, USA

Medical Imaging BMEN Spring 2016

SPECT QA and QC. Bruce McBride St. Vincent s Hospital Sydney.

Implementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system

Ch. 4 Physical Principles of CT

Nuclear Medicine Imaging

Fits you like no other

Corso di laurea in Fisica A.A Fisica Medica 5 SPECT, PET

Fits you like no other

Technical aspects of SPECT and SPECT-CT. John Buscombe

BME I5000: Biomedical Imaging

GPU implementation for rapid iterative image reconstruction algorithm

Emission Computed Tomography Notes

CT Basics Principles of Spiral CT Dose. Always Thinking Ahead.

ISO ISO ISO OHSAS ISO

Quantitative imaging for clinical dosimetry

Concepts, Applications, and Requirements for Quantitative SPECT/CT. Conflict of Interest Disclosure

Medical Image Analysis

Master of Science Thesis. Activity quantification of planar gamma camera images

If it matters to you, it matters to us

Workshop on Quantitative SPECT and PET Brain Studies January, 2013 PUCRS, Porto Alegre, Brasil Corrections in SPECT and PET

Small Angle Gamma Ray Scatter: What Is The Impact On Image Quality

Joint CI-JAI advanced accelerator lecture series Imaging and detectors for medical physics Lecture 1: Medical imaging

Assessment of OSEM & FBP Reconstruction Techniques in Single Photon Emission Computed Tomography Using SPECT Phantom as Applied on Bone Scintigraphy

AAPM Standard of Practice: CT Protocol Review Physicist

Monte-Carlo-Based Scatter Correction for Quantitative SPECT Reconstruction

8/2/2017. Disclosure. Philips Healthcare (Cleveland, OH) provided the precommercial

Positron Emission Tomography

Fast Timing and TOF in PET Medical Imaging

Positron. MillenniumVG. Emission Tomography Imaging with the. GE Medical Systems

IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 53, NO. 1, FEBRUARY

Spiral CT. Protocol Optimization & Quality Assurance. Ge Wang, Ph.D. Department of Radiology University of Iowa Iowa City, Iowa 52242, USA

Deviceless respiratory motion correction in PET imaging exploring the potential of novel data driven strategies

Medical Images Analysis and Processing

Mathematical methods and simulations tools useful in medical radiation physics

Quantitative capabilities of four state-of-the-art SPECT-CT cameras

Hybrid Imaging for Patient-Specific Dosimetry in Radionuclide Therapy

BIAS AND VARIABILITY IN IMAGE-BASED VOLUMETRIC YTTRIUM-90 DOSIMETRY

Nuclear Medicine Imaging Systems

Constructing System Matrices for SPECT Simulations and Reconstructions

3-D Monte Carlo-based Scatter Compensation in Quantitative I-131 SPECT Reconstruction

Shadow casting. What is the problem? Cone Beam Computed Tomography THE OBJECTIVES OF DIAGNOSTIC IMAGING IDEAL DIAGNOSTIC IMAGING STUDY LIMITATIONS

Image Acquisition Systems

DICOM. Supplement 188 Multi-Energy CT Imaging. DICOM Working Group 21 Computed Tomography

Corso di laurea in Fisica A.A Fisica Medica 4 TC

CT NOISE POWER SPECTRUM FOR FILTERED BACKPROJECTION AND ITERATIVE RECONSTRUCTION

V/Q Imaging Protocols

PURE. ViSION Edition PET/CT. Patient Comfort Put First.

CT Protocol Review: Practical Tips for the Imaging Physicist Physicist

Introduction to Biomedical Imaging

IMRT and VMAT Patient Specific QA Using 2D and 3D Detector Arrays

Optimization of CT Simulation Imaging. Ingrid Reiser Dept. of Radiology The University of Chicago

SPECT reconstruction

REMOVAL OF THE EFFECT OF COMPTON SCATTERING IN 3-D WHOLE BODY POSITRON EMISSION TOMOGRAPHY BY MONTE CARLO

Performance Evaluation of radionuclide imaging systems

The Effects of PET Reconstruction Parameters on Radiotherapy Response Assessment. and an Investigation of SUV peak Sampling Parameters.

QIBA PET Amyloid BC March 11, Agenda

Reconstruction from Projections

Symbia E and S System Specifications Answers for life.

Tomographic Reconstruction

A Comparison of the Uniformity Requirements for SPECT Image Reconstruction Using FBP and OSEM Techniques

MEDICAL IMAGE ANALYSIS

Design and performance characteristics of a Cone Beam CT system for Leksell Gamma Knife Icon

Digital Image Processing

in PET Medical Imaging

ATTENUATION CORRECTION IN SPECT DURING IMAGE RECONSTRUCTION USING INVERSE MONTE CARLO METHOD A SIMULATION STUDY *

Machine Learning for Medical Image Analysis. A. Criminisi

Mediso AnyScan S Single-Head and Dual-Head SPECT

4DM Packages. 4DM Packages & License Types. Information to help you order the appropriate licenses for your site.

Radiology. Marta Anguiano Millán. Departamento de Física Atómica, Molecular y Nuclear Facultad de Ciencias. Universidad de Granada

ML reconstruction for CT

Computer-Tomography I: Principles, History, Technology

Development and Performance of a Sparsity- Exploiting Algorithm for Few-View Single Photon Emission Computed Tomogrpahy (SPECT) Reconstruction

SPECT: Physics Principles and Equipment Design

Mediso AnyScan. Single-Head and Dual-Head SPECT

Validation of PET/CT dataset for radiation treatment planning

USING cone-beam geometry with pinhole collimation,

Venus Explorer Processing Technical specifications

3-D PET Scatter Correction

Semi-Quantitative Metrics in Positron Emission Tomography. Michael Adams. Department of Biomedical Engineering Duke University.

Computer-Tomography II: Image reconstruction and applications

PET/CT Image Segmentation using the Channeler Ant Model for Lymphoma Therapy Assessment

ANALYSIS OF CT AND PET/SPECT IMAGES FOR DOSIMETRY CALCULATION

Automated Image Analysis Software for Quality Assurance of a Radiotherapy CT Simulator

Dose Distributions. Purpose. Isodose distributions. To familiarize the resident with dose distributions and the factors that affect them

Continuation Format Page

Advanced Scatter Correction for Quantitative Cardiac SPECT

11/18/ CPT Preauthorization Groupings Effective January 1, Computerized Tomography (CT) Abdomen 6. CPT Description SEGR CT01

AIDR 3D Iterative Reconstruction:

Medical Image Processing in Nuclear Medicine. Andrew Todd-Pokropek University College London INSERM U494 Paris. Aims and Objectives

Design and Fabrication of Kidney Phantoms for Internal Radiation Dosimetry Using 3D Printing Technology

Transcription:

Educational Objectives SPECT/CT: Basics, Quality Assurance, and Clinical Applications 1. To understand the physics principles underlying SPECT/CT image acquisition and reconstruction 2. To understand the quality assurance procedures specific to SPECT/CT systems 3. To become familiar with clinical applications of SPECT/CT imaging Associate Professor, Department of Imaging Physics The University of Texas MD Anderson Cancer Center, Houston, Texas Spring AAPM Meeting March 2016 1 2 SPECT Single Photon Emission Computed Tomography Radio pharmaceutical administration injected, ingested, or inhaled Bio distribution of pharmaceutical uptake time Decay of radionuclide from within the patient the source of information SPECT Gamma camera detects radionuclide emission photons PET Coincidence ring detector detects annihilation photons Tomography performed to image the radio pharmaceutical distribution within the patient Used for visualization of functional information based on the specific radio pharmaceutical uptake mechanism Gamma Camera NaI(Tl) is the scintillator of choice High light output and High detection efficiency (~85% at 140 kev for 3/8 in. NaI) Good energy resolution (~10% at 140 kev) Large crystals (50 cm x 40 cm) Hygroscopic! Intrinsic Spatial and Energy Resolution # of scintillation photons, N Gamma ray energy, E Spatial Resolution = 100 /N 1/N 1/E Energy Resolution = 100 FWHM/E 1/E U of British Columbia 3 4 1

Collimators Collimators NaI Crystal NaI Crystal Absorptive Collimation Absorptive Collimation source source 5 6 Collimator Resolution Collimator Efficiency T D L e B L e H G F where C( D Le = fraction of 4 F = exposed fraction Parallel Hexagonal hole C = 3/8 ) 2 4 G CD L ( D T ) e 2 2 T D L e Collimator Resolution R g D( Le H B) L e System Resolution R R R 2 2 2 s i g Cherry, Sorenson, & Phelps, Physics of Nuclear Medicine, 2003 LEHR = 1.3x10 4 MELP = 3.1x10 4 Resolution is highest closest to the collimator therefore while imaging position patients as close as possible to collimator face 7 8 2

Sensitivity versus Source Distance Sensitivity: the detected photons count rate per unit activity [cps/uci] Photon flux vs. distance z 2 Crystal area vs. distance z 2 Overall sensitivity S z 2 z 2 constant z z = L e + H + B Anger Logic for Event Position Interaction location based on relative signal between X + and X (for X location) & Y + and Y (for Y location) X = (X + X )/(X + + X ) range 1 to +1 Y = (Y + Y )/(Y + + Y ) range 1 to +1 Interaction Energy Total Signal = X + + X + Y + + Y Y ( 1) (+1) Y Y+ Y+ (+1) R R R R X+ R R X R R X ( 1) 70 70 k 9 10 SPECT Acquisitions Wernick & Aarsvold, Emission Tomography, 2004 Yale School of Medicine SPECT acquires 2D projections of a 3D volume SPECT in the year 2000, JNMT 24:233, 2000 11 12 3

SPECT data corrections Measured Projections INT Uniformity Correction EXT Uniformity Correction SPECT in kbq/ml Scanner Calibration MHR/COR Inter-frame decay (some) Scatter Correction FBP/IR reconstruction CT Attenuation Correction SPECT in counts/ml Collimator Resolution Modelling 13 14 SPECT Iterative Recon: Scatter Modeling Scatter compensation occurs before attenuation the photopeak window contains scatter attenuation accounts for the removal of photopeak photons SPECT Acquisition Schema Circular versus (non circular) body contour orbit Step and Shoot versus Continuous Mode Adjacent energy window based estimate (DEW and TEW): Scatter estimated as a weighted sum of adjacent energy window images, Ci(x,y,) S(x,y,) = i k i C i (x,y,) Subtract scatter prior to reconstruction P corr (x,y,) P(x,y,) - S(x,y,) Incorporate scatter into forward projection P(x,y,) P corr (x,y,) + S(x,y,) 35000 30000 25000 20000 15000 10000 5000 0 In-111 Energy Spectrum #1 #2 0 50 100 150 200 250 300 Photon Energy (kev) TEW DEW 15 16 4

SPECT violates Radon transform angular symmetry Differential Attenuation L I( i ) b SPECT Acquisition Schema SPECT projections acquired over 360 degrees Exception: Cardiac SPECT acquired over 180 a i c I( i +) b I( i ) = I 0 e - a (L)dL c I( i +) = I 0 e - a (L)dL P() P(+) 0 0 180 Other mediating factors: distance dependent resolution depth dependent scatter Image courtesy Bill Erwin 17 18 SPECT Iterative Reconstruction Maximum Likelihood Expectation Maximization (ML EM) Ordered Subset Expectation Maximization (OS EM) Accounts for the statistical nature of photon detection Incorporates the system response p(b,d) the probability that a photon emitted from an object voxel b is detected by projection pixel d p(b,d) captures 1. Depth dependent resolution 2. Position dependent scatter 3. Depth dependent attenuation voxel: b pixel: d SPECT Iterative Reconstruction True projection intensity = sum of true voxel intensities weighted by detection probabilities True voxel intensity = sum of true detector intensities weighted by detection probabilities Forward Projection B b1 yd ( ) ( bpbd ) (, ) Back Projection D d1 () b y() d p(, b d) Use a measured attenuation map along with models of scatter and camera resolution to perform a far more accurate reconstruction 19 20 5

Iterative Reconstruction Flow Diagram SPECT Reconstructions IT=1 D [ k ] ( b) B d 1 [ k 1] b ' 1 ( b) D d 1 yd ( ) pbd (, ) [ k ] ( b') p( b', d) pbd (, ) IT=2 IT=3 FBP 360 0 FBP 180 0 In clinical practice, the stopping criteria is number of iterations (a time constraint) instead of a convergence criteria. IT=4 IT=16 IT=64 FBP noise IR noise 21 22 Hybrid SPECT/CT Motivation X ray transmission CT Improved speed (< 1 min) High resolution anatomical images Higher radiation dose Functional anatomical overlay (image fusion) Improve localization of uptake regions Increase confidence in interpretation HU to (CT AC) Transforms LaCroix et al., IEEE TNS 41, 1994 x( ECT) w( ECT) HU x 1000 w( ECT) HU x x( ECT) 1 w( ECT) K 1000 HUx w( ECT) x( E) x( E) 1 w( E) 1000 x( ECT) w( E) Photon energies different between CT and SPECT K 1 for Compton Scatter dominates low Z at ECT (low HU) K 1 for Photoelectric pernent for high Z at ECT (high HU) HU to transform is piece wise linear (bi or tri modal) 23 24 6

CT based AC for SPECT/CT Role of CT in SPECT/CT CT CT noise reduced Smooth, re bin CT to match SPECT Register CT w/ SPECT CT AC μ map Apply bi linear transform on pixel by pixel basis Two functions for CT as part of NM exams AC Anatomic Localization CT Dose Requirement Higher (Diagnostic ) Reconstructed SPECT Transition Matrix a ijk Other factors: SPECT projections Scatter estimates Collimator response The most important function of the CT component of a hybrid SPECT/CT scanner!!! Lower CT dose: Loss of anatomic and morphologic information Lower CT dose: Loss of SPECT accuracy from incorrect CT AC Moderate Ultra low (CT AC only) 25 26 SPECT/CT Quality Control Planar (AAPM Reports 6 and 9; NEMA NU 1 1994) Energy resolution (Intrinsic) Spatial resolution (Intrinsic and Extrinsic) Uniformity (Integral and Differential) Deadtime Sensitivity ( collimator) Pixel Size Rotational Uniformity and Sensitivity Variation Opposed Head Spatial Registration Multiple Energy Window Spatial Registration SPECT (AAPM Reports 22 and 52) Uniformity and Contrast (Image Quality) Resolution MHR/COR ( collimator) SPECT/CT (AAPM TG 177: Jim Halama) SPECT and CT image registration Image Quality (attenuation, scatter correction, iterative reconstruction) SPECT/CT: Image Registration To verify the electro mechanical registration of the isocenter and reconstructed field of view between the SPECT and CT images Does location (x, y, z) in SPECT image space spatially corresponds to location (x, y, z) in CT image space? SPECT/CT image registration is critical for Accurate SPECT images via CT based attenuation correction Display of fused images for clinical interpretation Does not address mis registration due to patient movement between SPECT and CT 27 28 7

Registration Test Setup A Acquire SPECT/CT scan of 3 point sources (capillary tubes) in air containing both CT contrast and Tc 99m solution Registration Test Setup A Acquire SPECT/CT scan of 3 point sources (capillary tubes) in air containing both CT contrast and Tc 99m solution CT image Fused SPECT/CT image Tc 99m CT contrast SPECT image 29 30 Registration Test Setup B Use Co 57 button sources w/ SPECT Jaszczak phantom containing Tc 99m water Co 57 emits 122 kev; Photopeak window 122 kev w/ 20% window Tc 99m emits 140 kev; Photopeak window 140 kev w/ 15% window 19% of counts in 57 Co energy window (110 134 kev) contained in 99m Tc energy window (129 150 kev) 35000 30000 25000 Image Registration Data Analysis Overlay re sampled SPECT and CT images in fused display For each of the 3 points determine the shift in (x, y, z) to match center of point source between SPECT and CT images Calculate the mean deviation between SPECT and CT images along any one direction as Mean deviation along x axis = (x 1 + x 2 + x 3 )/3 Similar for y and z 20000 Co-57 Tc-99m 15000 10000 5000 0 100 110 120 130 140 150 160 Photon Energy (kev) PASS criteria specifications TBD Mean deviation along any axis is less than one SPECT pixel used in routine clinical imaging 31 32 8

SPECT/CT: Image Quality ACR SPECT phantom ( Jaszczak ) with cold spheres and cold wedge section SPECT data acquisition based on ACR or AAPM Rpt 52 Use typical CT exam parameters used for SPECT/CT scans Reconstruct the SPECT data with iterative reconstruction using CT based AC, DEW scatter correction, and other routinely used reconstruction parameters Establish the baseline for image quality at Acceptance Test Evaluate the annual test results against baseline values Clinical SPECT/CT Imaging Radiopharmaceuticals available for SPECT/CT imaging Stress/Rest Myocardial Perfusion Imaging Stress: 99m Tc sestamibi or 99m Tc Tetrafosmin Rest: 99m Tc labeled agents or 201 Tl chloride 99m Tc MDP: bone diseases, bone metasteses 99m Tc MAA: perfusion 99m Tc sestamibi: parathyroid adenomas 99m Tc sulphur colloid: liver/spleen, lymphoscintigraphy 111 In Pentetreotide: neuroendocrine cancers 111 In ProstaScint: prostate cancer 123 I/ 131 I MIBG: pheochromocytoma, neuroblastoma 123 I/ 131 I NaI: thyroid cancer 99m Tc CEA: colorectal cancer 99m Tc RBCs: hemangioma 99m Tc HMPAO, ECD: brain perfusion 111 In WBC: infection 67 Ga citrate: inflammation, lymphoma 201 Tl chloride: tumor perfusion 153 Sm EDTMP: skeletal disease 89 SrCl: skeletal mets Some examples of clinical SPECT/CT imaging 33 34 99m Tc MDP Bone Planar Scan 99m Tc MDP Bone SPECT/CT Focal uptake in the L4 lumbar spine: Metastases? Trauma? Inflammation? Image courtesy Bill Erwin Degenerative joint disease (DJD) Bone metastases Image courtesy Bill Erwin 35 36 9

99m Tc sestamibi Parathyroid Imaging Ectopic parathyroid adenoma: What is the exact location for surgery? 90 Y microspheres Radioembolotherapy (Selective Internal RT) Hepatocellular Ca (TheraSphere, MDS Nordion) Colorectal Ca liver mets (SIR Spheres, SirTex) TheraSphere SIR Sphere 37 38 99m Tc MAA Pre Therapy SPECT/CT 90 Y dose calculation & safety assessment 99m Tc MAA SPECT/CT Catheter placement Extra hepatic shunting Lung shunting Perfusion (Hall et al., J Int Onc 2, 2009) 99mTc MAA SPECT/CT (20 min) 90Y SPECT/CT (35 min) Detection of Extra Hepatic MAA Shunting Sensitivity Specificity Planar 32 98 SPECT 41 98 SPECT/CT 100 93 (Ahmadzadehfar et al, JNM, 2010) (Siman et al, JNM 56, 2015) 39 40 10

Pre and Post 90 Y microsphere therapy PRIOR THERAPY POST 99m Tc MAA Lung Perfusion SPECT/CT: Lung Function based IMRT Planning Goal: lower radiation dose to functioning normal lung during IMRT of lung tumors by incorporating functional (in addition to anatomical) information in the treatment plan CT 3 June 2008 CT 5 Sept 2008 Pre IMRT Anatomical Plan Tc 99m MAA SPECT/CT provides perfusion image Perfusion image overlay on treatment planning CT Functional Plan Tc 99m MAA SPECT/CT 24 June 2008 90Y SPECT/CT 2 July 2008 Tc 99m MAA SPECT/CT 2 Sept 2008 Post IMRT = 50 th percentile contour (top 50% of pixels) = 90 th percentile contour (top 10% of pixels) Image courtesy Bill Erwin 41 42 153 Sm EDTMP Bone SPECT/CT: Internal Radionuclide Therapy Dosimetric imaging with 30 mci tracer dose Whole body planar images at 0, 2, 4, 24, 28, 48, and 52 hr SPECT/CT of target tumor at 24 hr to estimate tumor volume and absolute uptake Target tumor dose 40 Gy (w/ bladder & kidneys < 20 Gy) Whole body SPECT/CT 99m Tc MDP Bone Imaging Tumor Dose Estimate: Mass (M) = 0.683 kg (1 g/cc) Residence Time (T) = 10.7 h A (GBq) = 71.6 (or 1.935 Ci) Dose (E A T / M)= 172 Gy scaled to SPECT Ci @ 24 h Effective FIA(t) = FIA bio (t) e 0.693t/46.3h Image courtesy Bill Erwin 43 44 11

SPECT with contrast CT 99m Tc Sestamibi SPECT/CT Identification (NM) Multi phase IV contrast H&N CT Localization (Radiology) Synergy of SPECT/CT & contrast CT under clinical evaluation Clinical Benefits of SPECT/CT Visualization, diagnosis and interpretation of primary and metastases diseases Higher sensitivity and contrast than Planar imaging CT scan increases confidence in interpretation of SPECT examination Surgical planning IMRT treatment planning 90 Y microspheres therapy planning Internal radio pharmaceutical therapy planning 45 46 SPECT/CT: Limitations Patient motion Between SPECT and CT scans Respiratory and cardiac motion during SPECT acquisitions Contrast CT Contrast introduces electron density material mismatch map algorithms do not yet account for contrast CT Absolute quantification (Bq/mL) not yet fully developed Radionuclide dependent Acquisition/reconstruction technique dependent Calibration techniques not yet standardized Take home message s o p a s s é Nuclear Medicine often referred to as unclear Medicine SPECT/CT and PET/CT has changed the paradigm to New clear Medicine Imaging von Schulthess (MIB, 2004) 47 48 12