Direct MRI of Human Teeth using SWIFT

Slides:



Advertisements
Similar presentations
Pulse Timing parameters & Weighting
Advertisements

Fund BioImag : Echo formation and spatial encoding 1.What makes the magnetic resonance signal spatially dependent ? 2.How is the position of.
Assessment of tumoural ADC’s in rectal Tumours using Burst: New methodological Developments SJ Doran 1, ASK Dzik-Jurasz 2, J Wolber 2, C Domenig 1, MO.
Fund BioImag : Echo formation and spatial encoding 1.What makes the magnetic resonance signal spatially dependent ? 2.How is the position of.
Ari Borthakur, PhD Associate Director, Center for Magnetic Resonance & Optical Imaging Department of Radiology Perelman school of Medicine, University.
Magnetic Resonance Imaging
Imaging Sequences part I
MRI Phillip W Patton, Ph.D..
In Chan Song, Ph.D. Seoul National University Hospital
Richard Wise FMRI Director +44(0)
M R I Pulse Sequences Jerry Allison Ph.D..
BE 581 Lecture 3- Intro to MRI.
PHYSICS OF MAGNETIC RESONANCE
RF Pulse – generates a B 1 field that realigns the precessing spins in the low energy state In the case of a 90 o pulse the alignment is perpendicular.
MR TRACKING METHODS Dr. Dan Gamliel, Dept. of Medical Physics,
Parameters and Trade-offs
Topics spatial encoding - part 2. Slice Selection  z y x 0 imaging plane    z gradient.
Magnetic Resonance Imaging Maurice Goldman Member Académie des sciences.
Basic Principles MRI related to Neuroimaging Xiaoping Hu Department of Biomedical Engineering Emory University/Georgia Tech
The Basics of MRI The Basics of MRI. Current MRI technology displays images as multiple sets of gray tone images. Visualization and interpretation of.
Terry M. Button, Ph.D. Principals of Magnetic Resonance Image Formation.
Real-Time MRI – Outline Biomed NMR JF11/59 Technical Considerations - Data Acquisition - Image Reconstruction Preliminary Applications - Joint Movements,
Basics of Magnetic Resonance Imaging
Magnetic Resonance Imaging Basic principles of MRI This lecture was taken from “Simply Physics” Click here to link to this site.
Resonance condition. Pulse A coil of wire placed around the X axis will provide a magnetic field along the X axis when a direct current is passed through.
Psy 8960, Spring ‘07 Gradient and Spin Echoes1 Echoes, gradients and dephasing Gradient echoSpin echo.
Magnetic Resonance Imaging
Medical Imaging Systems: MRI Image Formation
Principles of MRI Physics and Engineering
What can you see by MRI ? Stephen Paisey.
Lung Imaging in the Mouse with SWIFT Curt Corum, Djaudat Idiyatullin, Steen Moeller, Ryan Chamberlain, Deepali Sachdev, and Mike Garwood Center for Magnetic.
Imaging Sequences part II
A new method for diffusion imaging using Burst excitation C. Wheeler-Kingshott 1, D. Thomas 2, M. Lythgoe 2, S. Williams 2 and S. J. Doran 1 1 University.
Medical Imaging Systems: MRI Image Formation
Basics of MRI.
Contrast Mechanism and Pulse Sequences Allen W. Song Brain Imaging and Analysis Center Duke University.
In Burst experiments, the read gradient is much larger then the other imaging gradients, hence, only translation along this gradient direction will cause.
Teeth Performed: Lubomir Kovalchuk. Teeth - bone formation in the oral cavity of vertebrates, and are used to rozkushuvannya chewing food, and to attack.
Contrast Mechanism and Pulse Sequences
NMR of SCI Using Nuclear Magnetic Resonance to Explore Spinal Cord Injury.
Low–field NMR (or MRI) Images of Laser polarized Noble Gas.
MRI Physics Dr Mohamed El Safwany, MD.. MRI Magnetic Resonance Imaging Magnetic Resonance Imaging.
3D sequence MRI in the assessment of meniscofemoral and ligament lesions of the knee MA.Chaabouni,A.Daghfous, A.Ben Othman,L.Rezgui Marhoul Radiology departement.
Functional Brain Signal Processing: EEG & fMRI Lesson 11 Kaushik Majumdar Indian Statistical Institute Bangalore Center M.Tech.
Sweep Imaging with Fourier Transform (SWIFT) in Breast Cancer
Magnetic Resonance Imaging of Fast Relaxing Spins: Acquisition during Adiabatic Excitation November 14, 2005, CMRR : Djaudat Idiyatullin.
1. Introduction Magnetic resonance spectroscopy (NMR) and imaging (MRI) are safe and highly versatile modalities, based on fundamental concepts in quantum.
Continuous SWIFT Djaudat Idiyatullin. , Steven Suddarth+, Curt Corum
MRI: Contrast Mechanisms and Pulse Sequences
Magnetic Resonance Learning Objectives
Principles of MRI Physics and Engineering Allen W. Song Brain Imaging and Analysis Center Duke University.
In vivo MRI of Fast Relaxing Spins Using a Swept Radiofrequency Djaudat Idiyatullin, Curt Corum, Jang-Yeon Park, Michael Garwood Center for Magnetic Resonance.
 This depends on a property of nuclei called spin.  Gyroscope: Principle: As long as its disc remains spinning rapidly the direction of the spin axis.
MAGNETIC RESONANCE IMAGING by PRADEEP V.EPAKAYAL. Mem.no L.
SWIFT Dual Breast Imaging Sequence and Coil with Interleaved Adiabatic Fat Suppression high temporal and spatial resolution #3369 Computer 8 breast imaging.
BOLD functional MRI Magnetic properties of oxyhemoglobin and deoxyhemoglobin L. Pauling and C. Coryell, PNAS USA 22: (1936) BOLD effects in vivo.
Dipole Matched Filter with SWIFT Curt Corum, Djaudat Idiyatullin, Steen Moeller, Ryan Chamberlain, and Mike Garwood Center for Magnetic Resonance Research.
DENTISTRY.
FMRI data acquisition.
MRI Physics in a Nutshell Christian Schwarzbauer
Where Mt is the magnetization at time = t, the time after the 90o pulse, Mmax is the maximum magnetization at full recovery. At a time = one T1, the signal.
Physics of Magnetic Resonance Imaging
An Optimal Design Method for MRI Teardrop Gradient Waveforms
Parallel Imaging Artifacts in Body Magnetic Resonance Imaging
10.5 Fourier Transform NMR Instrumentation
Magnetic Resonance Imaging
(4)ELECTRONIC SUPPORT SYSTEM
Superconducting Magnets
The echo time (TE) The echo time (TE) refers to the time between the application of the radiofrequency excitation pulse and the peak of the signal induced.
T2 Relaxation Time T2 relaxation time is defined as the time needed to dephase up to 37% of the original value. T2 relaxation refers to the progressive.
Presentation transcript:

Direct MRI of Human Teeth using SWIFT Djaudat Idiyatullin, Curt Corum, Adeka McIntosh, Steen Moeller, and Michael Garwood Center for Magnetic Resonance Research (CMRR), Department of Radiology University of Minnesota Medical School, Minneapolis, Minnesota, USA Djaudat Idiyatullin, Curt Corum, Adeka McIntosh, Steen Moeller, Michael Garwood Direct MRI of Human Teeth by SWIFT. At Joint Annual Meeting ISMRM-ESMRMB May 19- May 25, 2007, Berlin, Germany.

1H NMR relaxation properties a tooth Enamel T2 ~70 μs Organic matter and water ~14% by wt. Dentin Organic matter and water ~35% by wt. T2 multi exponential : ~220 μs (28%) ~ 56 μs ( 7%) ~ 12 μs (56%) T1: ~100 ms Cementum T2 ~70 μs ? Organic matter and water ~55% Pulp T2 > 1 ms Connective tissue, vessels and nerves. Only the pulp is visible by conventional MRI. Images of enamel, dentin and cementun have been obtained only by solid-state MRI in vitro.

Reported MRI of Teeth: SPI (Single Point Imaging): Lockhart et al., Proc Finn Dent Soc., (1992) Appel and Baumann, Oral Surgery, Oral Medicine, Oral Pathology, Oral Radiology & Endodontics, (2002) STRAFI (Stray-field imaging): Baumann et al., Oral Surgery, Oral Medicine…, (1993) BLAST (Projection MRI): Wu et al., Proc Natl Acad Sci U S A, (1999) FLASH (“Liquid” sequences): Tutton et al., Br J Radiol, (2002) Olt et al., Magn Reson Med, (2004) Gahleitner et al., Rofo, (1998) Lloyd et al., Caries Research, (2000) UTE Gatehouse and Bydder, Clinical Radiology, (2003) SWIFT…

Challenges for direct in vivo MRI of teeth Range of 1H relaxation times (T2): ~ 10 – 100 μs Any echo based sequence unusable! Total acquisition time: for in vivo experiments ~10 minutes SPI and Stray-field imaging impractical! Peak RF power limit (for broadband excitation): Projection MRI (BLAST) impractical?

SWeep Imaging with Fourier Transform (SWIFT) D. Idiyatullin, C. Corum, J.-Y. Park, M. Garwood, Fast and quiet MRI using a swept radiofrequency, Journal of Magnetic Resonance 181, (2006) 342-349.

SWeep Imaging with Fourier Transform (SWIFT) D. Idiyatullin, C. Corum, J.-Y. Park, M. Garwood, Fast and quiet MRI using a swept radiofrequency, Journal of Magnetic Resonance 181, (2006) 342-349.

SWeep Imaging with Fourier Transform (SWIFT) D. Idiyatullin, C. Corum, J.-Y. Park, M. Garwood, Fast and quiet MRI using a swept radiofrequency, Journal of Magnetic Resonance 181, (2006) 342-349.

Direct MRI of a tooth (in vitro) demineralization pulp plaque dentin cementum root sagittal 3D MRI of decayed molar tooth obtained with SWIFT sw = 62.5 kHz, 4.7 T, 10 min.

Direct MRI of a tooth (in vitro) demineralization dentin pulp root coronal 3D MRI of decayed molar tooth obtained with SWIFT sw = 62.5 kHz, 4.7 T, 10 min.

Direct MRI of a tooth (in vitro) Mip and rotation 3D MRI of decayed molar tooth obtained with SWIFT sw = 62.5 kHz, 4.7 T, 10 min.

4 T 1H Quadrature microstrip-loop RF surface coil for dental imaging RF field penetration of the coil in three orthogonal directions 30 cm

Selected slices of 3D images of a normal mandible and surrounding area Selected slices of 3D images of a normal mandible and surrounding area. (4T). LOOK MOM, NO CAVITIES! Gradient-echo 2.5 min sw = 80 kHz, TE = 3ms 256 x 256 x 64 SWIFT 3 min sw = 62 kHz, 256 x 256 x 64

Fillings and crowns in SWIFT images Ceramic crown covering two teeth Dental cement filling (Filling compounds T2 slightly longer than T2 of dentin, or proton density higher?) (In SWIFT images, the ceramic crown does not create a pronounced susceptibility artifact)

Direct MRI of a tooth under “in vivo conditions” Tooth surrounded by sponge in water, 4 T human magnet, total FOV diameter 15cm demineralization 3D FLASH (15 min) TE=3ms sw = 80 kHz 3D SWIFT, orthogonal slices, (10 min) sw = 62.5 kHz

In-vivo conditions, varying bandwidth (sw) sw = 125 kHz sw = 62.5 kHz sw = 31 kHz Tooth surrounded by sponge in water, 4 T human magnet, 3D SWIFT, total FOV diameter 15cm, (10 min)

Conclusions Direct MRI of teeth is feasible with SWIFT Demineralization and associated Decay are easily visible, (First observation of MRI contrast in deminerized tooth?) The SWIFT sequence appears well suited to studying the progress of dental caries and for early stage diagnosis of dental caries.

More SWIFT 1669. Signal Processing and Image Reconstruction for SWIFT 1670. Progress in Rapid and Short Acquisition Delay Imaging with SWIFT 3805. Ultrastructural Organization of Bone and Tendon – Novel Method for Musculoskeletal Imaging of Extremely Fast Relaxing Spins Acknowledgments. We gratefully acknowledge support by NIH grants 5R01CA092004 and 5P41RR008079, the Keck Foundation. Thanks to many others at the CMRR!

End

The advantages of SWIFT fast; The method avoids delays for gradient switching, and also time for the excitation pulse (it’s combined with the acquisition period). (b) sensitive to short T2 ; any T2 > 1/sw. (c) reduced motion artifacts; Because the SWIFT method has no “echo time” it is expected to be less sensitive to motion and flow artifacts than conventional MRI methods. (d) reduced signal dynamic range; The different frequencies are excited sequentially the resulting signal is distributed in time, leading to a decreased amplitude of the acquired signal. This allows more effective utilization of the dynamic range of the digitizer. (e) quiet. The SWIFT method uses a small step when changing gradients between projections, and the fast gradient switching that creates loud noise can be avoided.

Direct MRI of the teeth (in vitro) Two hours after extraction sw = 62 kHz, 4.7 T Dried (Three month in room temperature) sw = 125 kHz, 9.4 T

SWeep Imaging with Fourier Transform (SWIFT) D. Idiyatullin, C. Corum, J.-Y. Park, M. Garwood, Fast and quiet MRI using a swept radiofrequency, Journal of Magnetic Resonance 181, (2006) 342-349. Animate this ***

Direct MRI of a tooth (in vitro) demineralization pulp cementum plaque root dentin 3D MRI of decayed molar tooth obtained with SWIFT sw = 62.5 kHz, 4.7 T, 10 min.