Magnetic Resonance Imaging. Qun Zhao Bioimaging Research Center University of Georgia

Similar documents
BMB 601 MRI. Ari Borthakur, PhD. Assistant Professor, Department of Radiology Associate Director, Center for Magnetic Resonance & Optical Imaging

Part III: Sequences and Contrast

The physics US and MRI. Prof. Peter Bogner

The Basics of Magnetic Resonance Imaging

Contrast Mechanisms in MRI. Michael Jay Schillaci

MRI Physics I: Spins, Excitation, Relaxation

MRI in Practice. Catherine Westbrook MSc, DCRR, CTC Senior Lecturer Anglia Polytechnic University Cambridge UK. John Talbot MSc, DCRR

Magnetic Resonance Imaging. Pål Erik Goa Associate Professor in Medical Imaging Dept. of Physics

Nuclear Magnetic Resonance Imaging

MRI in Review: Simple Steps to Cutting Edge Part I

Cambridge University Press MRI from A to Z: A Definitive Guide for Medical Professionals Gary Liney Excerpt More information

Medical Imaging Physics Spring Quarter Week 9-1

FREQUENCY SELECTIVE EXCITATION

EL-GY 6813/BE-GY 6203 Medical Imaging, Fall 2016 Final Exam

Introduction to MRI. Spin & Magnetic Moments. Relaxation (T1, T2) Spin Echoes. 2DFT Imaging. K-space & Spatial Resolution.

Physics and Brain Imaging

Magnetic Resonance Imaging

Basic MRI physics and Functional MRI

Magnetic Resonance Imaging (MRI)

The physics of medical imaging US, CT, MRI. Prof. Peter Bogner

NMR/MRI examination (8N080 / 3F240)

Lecture 12 February 11, 2016

Field trip: Tuesday, Feb 5th

Fundamental MRI Principles Module Two

Introduction to the Physics of NMR, MRI, BOLD fmri

The NMR Inverse Imaging Problem

Magnetic Resonance Imaging

Quantitative Susceptibility Mapping and Susceptibility Tensor Imaging. Magnetization and Susceptibility

Introduction to Nuclear Magnetic Resonance Spectroscopy

Bioengineering 278" Magnetic Resonance Imaging" " Winter 2011" Lecture 9! Time of Flight MRA!

Introduction to Biomedical Imaging

Blood Water Dynamics

Fundamental MRI Principles Module 2 N. Nuclear Magnetic Resonance. X-ray. MRI Hydrogen Protons. Page 1. Electrons

Physics of MR Image Acquisition

Applications of Spin Echo and Gradient Echo: Diffusion and Susceptibility Contrast

Magnetic Resonance Imaging

Part II: Magnetic Resonance Imaging (MRI)

Introduction to Magnetic Resonance Imaging (MRI) Pietro Gori

Magnetic resonance imaging MRI

MRS: IN VIVO SPECTROSCOPIC IMAGING MAIN POINTS

Chapter 14:Physics of Magnetic Resonance

Introduction to MRI Acquisition

Rad 226b/BioE 326b In Vivo MR: Relaxation Theory and Contrast Mechanisms

Biomedical Imaging Magnetic Resonance Imaging

How does this work? How does this method differ from ordinary MRI?

Physical fundamentals of magnetic resonance imaging

G Medical Imaging. Outline 4/13/2012. Physics of Magnetic Resonance Imaging

Introduction to Magnetic Resonance Imaging

Spatial encoding in Magnetic Resonance Imaging. Jean-Marie BONNY

HY Ιατρική Απεικόνιση. Διδάσκων: Kώστας Μαριάς

Dynamic Contrast Enhance (DCE)-MRI

Quantitative MRI & Dynamic Models

Chemical Exchange. Spin-interactions External interactions Magnetic field Bo, RF field B1

Principles of MRI EE225E / BIO265. Instructor: Miki Lustig UC Berkeley, EECS

A Hands on Introduction to NMR Lecture #1 Nuclear Spin and Magnetic Resonance

Advanced Topics and Diffusion MRI

RADIOLOGIV TECHNOLOGY 4912 COMPREHENSEIVE REVIEW/MRI WORSHEET #1- PATIENT CARE AND SAFETY/PHYSICAL PRINCIPLES

MRI Physics (Phys 352A)

Magnetic Resonance Spectroscopy

How is it different from conventional MRI? What is MR Spectroscopy? How is it different from conventional MRI? MR Active Nuclei

Physics in Clinical Magnetic Resonance Spins, Images, Spectra, and Dynamic Nuclear Polarization

Sensitivity Enhancement and Fast NMR BCMB 8190

Spatial encoding in Magnetic Resonance Imaging. Jean-Marie BONNY

The ASL signal. Parenchy mal signal. Venous signal. Arterial signal. Input Function (Label) Dispersion: (t e -kt ) Relaxation: (e -t/t1a )

Introduction to NMR! Ravinder Reddy!

Introduction to the Course and the Techniques. Jeffry R. Alger, PhD Ahmanson-Lovelace Brain Mapping Center Department of Neurology

MRI Physics II: Gradients, Imaging. Douglas C. Noll, Ph.D. Dept. of Biomedical Engineering University of Michigan, Ann Arbor

Rad Tech 4912 MRI Registry Review. Outline of the Registry Exam: Certification Fees

M R I Physics Course. Jerry Allison Ph.D., Chris Wright B.S., Tom Lavin B.S., Nathan Yanasak Ph.D. Department of Radiology Medical College of Georgia

MRI Fundamentals. Class II (MR Principles)

MOLECULAR SPECTROSCOPY AND PHOTOCHEMISTRY

MR Spectroscopy: The Physical Basis and Acquisition Strategies

2.1.1 A Brief History of NMR The conception of NMR sprouted after the Pauli s prediction of nuclear spin in

PhD THESIS. prepared at INRIA Sophia Antipolis

NMR and MRI : an introduction

Principles of Magnetic Resonance Imaging

The Theory of Nuclear Magnetic Resonance Behind Magnetic Resonance Imaging. Catherine Wasko Physics 304 Physics of the Human Body May 3, 2005

NMR Imaging in porous media

ENG4BF3 Medical Image Processing

MRI. made. likely simplistic. Sorry, guys! We have less than one hour! Part 2: Sources of contrast. Endogenous (tissue) contrast

Diffusion Tensor Imaging I: The basics. Jennifer Campbell

New developments in Magnetic Resonance Spectrocopy and Diffusion MRI. Els Fieremans Steven Delputte Mahir Ozdemir

Sketch of the MRI Device

Principles of EPR and Image Acquisition

PETER PAZMANY CATHOLIC UNIVERSITY Consortium members SEMMELWEIS UNIVERSITY, DIALOG CAMPUS PUBLISHER

BNG/ECE 487 FINAL (W16)

Me myself and MRI: adventures in not understanding nuclear physics.

ADIABATIC PULSE PREPARATION FOR IMAGING IRON OXIDE NANOPARTICLES

Technical University of Denmark

With that first concept in mind, it is seen that a spinning nucleus creates a magnetic field, like a bar magnet

Electrical Engineering 3BA3: Structure of Biological Materials

Rochester Institute of Technology Rochester, New York. COLLEGE of Science Department of Chemistry. NEW (or REVISED) COURSE:

QUALITY ASSURANCE OF MAGNETIC RESONANCE IMAGING FOR ADAPTIVE RADIOTHERAPY: PRELIMINARY INVESTIGATIONS TREVOR THANG 1 Supervisors: Dr.

Functional Magnetic Resonance Imaging (FMRI) is an imaging technique for

BME I5000: Biomedical Imaging

Magnetic Resonance Elastography for Liver Fibrosis. By: Larissa Schudlo and Natalie Tong

Outlines: (June 11, 1996) Instructor:

Welcome to MR! CT PET (with FDG) MRI (T2 w.) MR Image types: T2 weighted T1 weighted Sequence parameters FLAIR Diffusion

MRI Homework. i. (0.5 pt each) Consider the following arrangements of bar magnets in a strong magnetic field.

Doppler echocardiography & Magnetic Resonance Imaging. Doppler echocardiography. History: - Langevin developed sonar.

Transcription:

Magnetic Resonance Imaging Qun Zhao Bioimaging Research Center University of Georgia

The Nobel Prize in Physiology or Medicine 2003 "for their discoveries concerning magnetic resonance imaging" Paul C. Lauterbur Sir Peter Mansfield

The Nobel Prize in Physiology or Medicine 2003 Lauterbur Magnetic field gradient encoding Peter Mansfield Echo planar imaging 1976

Imaging System: 7T-160 mm Magnets are often horizontal bore Coils built to order

Imaging System: 7T-210 mm Imaging methods include 1. Relaxometric measurements (T1, T2 and T2* mapping) 2. Quantitative diffusion mapping (DWI) and diffusion tensor imaging (DTI) 3. Quantization of vascular leakiness and permeability of tumor tissue 4. Spectroscopic imaging of 1H metabolites to monitor cellular response to therapy 5. 1H Single voxel spectroscopic measurements 6. Blood flow measurements using ASL (arterial spin labeling) technique 7. BOLD (blood oxygen level dependent contrast) measurements for fmri studies

RF coils are quite varied Transmit coils and gradient coils are often fixed in the bore much like a high resolution system Observe coils may be localized on animal like these surface coils From Doty Scientific

Human MRI 3T: 60cm Surface or volume coil UGA 3 Tesla magnet

General Imaging System Components (From Joy Hirsh, Columbia University)

Source of MR signal At rest, atoms align parallel to magnetic field. Lowest energy state. After RF absorption, net magnetization is orthogonal to magnetic field RF emission at Larmor frequency RF signal decays with time as atoms realign (relaxation). Antennas can measure this emission. 9

Simple Imaging Strategy During gradient spins in each volume element have their own precession frequency Can get a 1D image of sample used in gradient shimming High positive frequency Zero frequency Z High negative frequency

Field Strength Example: Slice Selection Gradient at 3T Gradients make field stronger at one location compared to another. Larmor frequency different along this dimension. RF pulse only energizes slice where field strength matches Larmor frequency. 127 Mhz RF pulse Larmor Freq 126 Mhz 127 Mhz 128 Mhz 11 Z Position

Y Position Phase encoding gradient Orthogonal gradient applied between RF pulse and readout This adjusts the phase along this dimension. Analogy: Phase encoding is like timezones. Clocks in different zones will have different phases. 12 Field Strength

Simple 2D Image For 2D imaging use gradients in different directions (x, z) in different evolution periods (t1, t2) 90x Gz t1 t2 Gx z 1 x 2

Echo Planar Imaging Speeding up Acquisitions 90x Gz t2 t2 t2 t2 t2 dw-1 dw-2 dw-3 dw-4 dw-5 t1 t2 will have spatial image (needs to be reversed in even dw) t1 can sample a number of different properties t1 could have a gradient in another dimension 2D map t1 could sample chemical shift dispersion - MRSI

Fourier Transform in k Space k(t) = t (db/dx) dt ( x) S( k) e i2 kx dk 1. A simple circle at the center of the image space and the representation of the circle in k-space. Note that the k-space has the greatest intensity at the center. 2. Additional of a second circle to the image space introduces a grating pattern to the k-space. 3. An image of the brain contains much more spatial information, with much more complex k-space representation

More about Raw MRI image: K-Space 16 Source: Traveler s Guide to K-space (C.A. Mistretta)

MR Contrast Agents In MRI, contrast agents are usually used to improve the visibility of diseased tissues. T1 contrast CA: increase R1 relaxation rate, e.g. Gadolinium (Gd), Mn 2+ T2 contrast CA: increase R2 rate, e.g. iron oxide nanoparticles Chemical exchange saturation transfer (CEST) CA: nucleus exchange b/w two or more chemical environment intra- or inter-molecularly Heteronuclear contrast CA: non-proton based, e.g. 19F, 129 Xe, or 13C

Mn 2+ Enhanced MRI of Mouse Brain Figure 1. Typical horizontal (left), sagittal (center), and axial (right) cuts from a T1-weighted spin-echo 3D-MEMRI of a mouse brain. Resolution is approximately 100. 11.7T system. (Lee, Silva, Merkle, Koretsky, (2005) Mag. Res. In Med. 53, 640-648.

Contrast Agents based on Gd 3+ Gd 3+ is has electron spin 7/2 Shortens T1, T2 of water protons T1 weighted image enhances areas of binding This construct targets areas of inflammation Boutry et al., Magn. Reson. Med. 53: 800-807 (2005)

Magnetic resonance imaging of cell surface receptors using targeted contrast agents, D. Artemov, Z.M. Bhujwalla, J.W.M. Bulte, Current Pharm. Biotech. 5:485-494.

Vascular Architecture can be Imaged Figure 1. Rat hindquarters using a contrast agent injected Into the blood stream. 7T system. (Varian website)

Dynamic contrast enhanced MRI for canine brain tumor 1. Seven brain tumors enhanced with Gd-DTPA Enhancement curves Kinetic modeling: Kel, Kep 2.Brain mass case study Multiparametric MRI: structural, DCE-MRI, DW-MRI, MRS Zhao, et al. Vet. Radio & Ultrasound, 2009

T2 Contrast agents T2 contrast agent: increase R2 rate, e.g. iron oxide nanoparticles. TEM images of Fe 3 O 4, CoFe 2 O 4, and MnFe 2 O 4 Category Nano-particles: Mono-disperse (non-aggregated) iron oxide core (<20nm) Ultra-small iron oxide: Mono-disperse (<50nm) Super-Paramagnetic Iron Oxide (SPIO) Aggregated iron oxide core (>50nm) Properties Highly susceptible to magnetic fields and therefore easily magnetized Applications: tracking/monitoring of labeled stem/tumor cells

Origin of Bulk Susceptibility Effects All materials have a magnetic susceptibility, We can assign such a susceptibility to each volume element In the presence of a magnetic field each has an induced dipole moment, B 0. Fields from these dipoles cancel in the interior of material, but they do not at surfaces Hence shape dependent corrections Total field B = B 0 [1 + (4 /3 - ) ] = -2 = 4 /3

Quantification of iron concentration: T 2 * Relaxometry Can infer agent concentration from relaxation rates Basic premise is to observe the increase in relaxation rate with the Fe-based agent relaxivity known. R * 2 R * 20 Applies to T 2 or T 2 * Experimental evidence shows relaxation rate is approximately linear at low concentration r Fe C Picture adapted from Liu et al Magn Reson Med. 2009 Apr;61(4):761-6

Visualizing Implanted Stem Cells These cells are labeled with iron oxide nanoparticles and cells have been injected into a mouse heart. Data are from a 7T MRI system. (Kustermann et al. (2005) NMRIn Biomedicine, 18, 362-370)

(MRSI) Magnetic Resonance Spectroscopy Imaging Prostate Cancer B- Spectral Grid C- MRSI Array Swanson et al. Cancer Investigation 19, 510-523 (2001)

MRS in Monitoring Disease Progression: a Mouse Model of Alzheimer s Disease Figure 1. Changes in brain metabolites as a function of age. 9.4T study on 18 L voxels. Myoinositol is also seen in APP-PS1 mice. (Marjanska,, Ugurbil, Garwood, (2005) PNAS 102, 11906-11910.