Active Detuning of Inductively Coupled Surface Coils Jolinda Smith Lewis Center for Neuroimaging University of Oregon.

Slides:



Advertisements
Similar presentations
Fund BioImag : Echo formation and spatial encoding 1.What makes the magnetic resonance signal spatially dependent ? 2.How is the position of.
Advertisements

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.
BOLD Imaging at 7T Mark Elliott CfN Symposium 4/9/2008.
MRI Acquisition Methods for Brain Morphometry
Magnetic Resonance Imaging
MRI Phillip W Patton, Ph.D..
Richard Wise FMRI Director +44(0)
NON-EXPONENTIAL T 2 * DECAY IN WHITE MATTER P. van Gelderen 1, J. A. de Zwart 1, J. Lee 1,3, P. Sati 1, D. S. Reich 1, and J. H. Duyn 1. 1 Advanced MRI.
PHYSICS OF MAGNETIC RESONANCE
Six-week project Lauren Villemaire MBP 3970Z Department of Medical Biophysics University of Western Ontario.
Statistical Parametric Mapping
MICE RF and Coupling Coil Module Outstanding Issues Steve Virostek Lawrence Berkeley National Laboratory MICE Collaboration Meeting October 26, 2004.
Parameters and Trade-offs
Basic Principles MRI related to Neuroimaging Xiaoping Hu Department of Biomedical Engineering Emory University/Georgia Tech
[1] Gold, G. et al., Proc. ISMRM, 84, [2] Scott, G. et al., Proc. ISMRM, 20, [3] Atalar, E. et al., MRM, 36: 596, [4] Quick, H. et al.,
Bruce Fischl MGH ATHINOULA A. MARTINOS CENTER Harvard Medical School MIT CSAIL/HST some open issues in functional MRI (thanks to Larry Wald for almost.
A SADDLE QUADRATURE RF COIL for IN VIVO RODENT IMAGING at 21.1 T Jose A. Muniz 1,2, Jens T. Rosenberg 1,2 & S.C. Grant 1,2 1 The National High Magnetic.
23 October 2005MICE Meeting at RAL1 MICE Tracker Magnets, 4 K Coolers, and Magnet Coupling during a Quench Michael A. Green Lawrence Berkeley Laboratory.
FMRI: Biological Basis and Experiment Design Lecture 10: The Dreaded Drop-out Spin echo review Field maps Through-slice dephasing © Melissa Tillery
Noise near peak field is increased Peak width narrow Peak is symmetric Purpose: Resonate nuclei to prevent polarization. Matching the resonant frequencies.
FT-NMR.
Circuitry of the Electric Guitar Eric Johnsen. The Magnetic Pickup  Voltage generator  Inductive coil around magnet Picks up fluctuations in the magnetic.
FMRI: Biological Basis and Experiment Design Lecture 12: Signal-to-Noise Ratio Things that determine signal strength –voxel size –RF coil Things that determine.
FMRI: Biological Basis and Experiment Design Lecture 8: Pulse sequences, Take 2 Gradient echo review K-space review Slice selection K-space navigation.
G Practical MRI 1 Receive Arrays.
SPIN 2004 Oct. 14, 2004 W. Kim, S.S. Stepanyan, S. Woo, M. Rasulbaev, S. Jin (Kyungpook National University) S. Korea Polarization Measurements of the.
RF Coils Used In MRI.
Magnetic Resonance Imaging 4
대구가톨릭대학병원 영상의학과 이 영 환 M M R R Basic Physics. MR Signal T1-, T2-weighted TR, TE MR Signal T1-, T2-weighted TR, TE.
Principles of MRI Physics and Engineering
What can you see by MRI ? Stephen Paisey.
Motors Make the world go ‘round By Jackson Greer, Room 305.
Sylwia Heinze-Paluchowska Department of Magnetic Resonance Imaging (NZ56)
Basics of MRI.
2 High Resolution T2 Imaging Rat versus Mouse T1 MP-RAGE Dark CSF Resolution Rat: 156 x 156 x 700 µ m 3 Mouse: 138 x 117 x 400 µm 3 Coil setup: Transmit:Integrated.
Basics of Functional Magnetic Resonance Imaging. How MRI Works Put a person inside a big magnetic field Transmit radio waves into the person –These "energize"
Comparison of Surface Coil and Automatically-tuned, Flexible Interventional Coil Imaging in a Porcine Knee R. Venook 1, B. Hargreaves 1, S. Conolly 1,
MR Scanner Transmit Gain as an Indicator For Lead Heating November, 2006.
Allen W. Song, PhD Brain Imaging and Analysis Center Duke University MRI: Image Formation.
High Resolution 3D Diffusion Pulse Sequence Dept. of Radiology Medical Imaging Research Lab. University of Utah Eun-Kee Jeong, Ph.D. Ph.D. Seong-Eun Kim,
NMR of SCI Using Nuclear Magnetic Resonance to Explore Spinal Cord Injury.
Brit and the Rad Lab at MIT Radiation Laboratory Series: Documented developments from the Rad Lab Volume 19 (copyright 1949): Waveforms- edited by B. Chance.
11 April, 2003 PMRIL Autotuning Interventional Coils for Imaging Ross Venook, Greig Scott, Garry Gold & Bob Hu.
Functional Brain Signal Processing: EEG & fMRI Lesson 11 Kaushik Majumdar Indian Statistical Institute Bangalore Center M.Tech.
Spatial and temporal limits of fMRI Menon RS, Kim SG. Spatial and temporal limits in cognitive neuroimaging with fMRI. Trends Cogn Sci Jun;3(6):
RT 4912 Review (C) Rex T. Christensen MHA RT (R) (MR) (CT) (ARRT) CIIP.
Autotuning Electronics for Varactor Tuned, Flexible Interventional RF Coils Ross Venook, Greig Scott, Garry Gold, and Bob Hu.
MRI Magnetic Resonance Imaging. Definition A non-ionizing technique with full three dimensional capabilities, excellent soft-tissue contrast, and high.
Receive Coil Arrays and Parallel Imaging for fMRI of the Human Brain
Real time shimming (RTS) for compensation of respiratory induced field changes P van Gelderen, JA de Zwart, P Starewicz, RS Hinks, JH Duyn Introduction.
Hanyang University 1/17 Antennas & RF Devices Lab. MODERN ANTENNA HANDBOOK by CONSTANTINE A.BALANIS ch. 4.4 – Jeong Gu Ho.
FMRI data acquisition.
CLARIDGE CHAPTER 2.2; 3.2.
Sunday Case of the Day Physics
DALHM Progress Meeting September 2003
MRI Physics in a Nutshell Christian Schwarzbauer
A new RF transmit coil for foot and ankle imaging at 7T MRI
Physics of Magnetic Resonance Imaging
Magnetic Resonance Imaging
Image construction. Image construction. (A) Step 1: Slice selection. A slice-selecting gradient (GS) is applied at the same time as the excitatory radiofrequency.
Introduction to Magnetic Resonance Spectroscopy
Basics of fMRI and fMRI experiment design
Pulse sequence diagrams show the benefits of parallel imaging for DWI
(4)ELECTRONIC SUPPORT SYSTEM
Superconducting Magnets
RF Coils in MRI By: Jamil Abdolmohammadi MSc of MRI
Left, T1 spin-echo image at 1
Same section position with spin-echo T1-weighted sequences at 1
Presentation transcript:

Active Detuning of Inductively Coupled Surface Coils Jolinda Smith Lewis Center for Neuroimaging University of Oregon

Inductive coupling Tuned coil is inductively coupled to a matching loop No physical connection to tuned coil

Inductive coupling Easy to construct Balanced Especially useful for implanted and cryocooled coils Kuhns, P. L., M. J. Lizak, et al. (1988). "Inductive Coupling and Tuning in Nmr Probes - Applications." Journal of Magnetic Resonance 78(1): Hoult, D. I. and B. Tomanek (2002). "Use of mutually inductive coupling in. probe design." Concepts in Magnetic Resonance 15(4):

Need for decoupling When using separate transmit and receive coils, they must be decoupled from each other. Failure to do so results in nonuniform flip angles and image artifacts. DecoupledNot decoupled

Approaches to decoupling Geometric decoupling Passive detuning with crossed diodes Optical detuning with photodiodes Active detuning with pin diodes

Pin diode detuning Active detuning uses pin diodes to detune the receive coil during the transmit phase. Biasing pin diode creates resonant circuit; coupling to this circuit shifts resonance of coil L C

Use a third coil Third coil is switched into resonance by biasing on a pin diode Coupling of detuning coil with receive coil shifts resonance peak Analogous to pin diode detuning of capacitively coupled coils Wong W H, Rath A R, “Detunable coil assembly and method of detuning RF coil for MRI”, US Patent no. 6,552,544 (2003)

Inductively coupled coil with active detuning Receive coil diameter = 1 inch Detuning coil diameter = 1.25 inches Pickup coil diameter = 0.75 inches Height of stack = 0.5 inches Pin diode off Pin diode on

Inductively coupled coil with Helmholtz pair transmit With detuningWithout detuning -26 dB -51 dB S 21, transmit coil on port 1, receive coil on port 2 Spin echo images of water- filled phantom

Inductively coupled coil with birdcage transmit coil Without detuningWith detuning -15 dB -49 dB S 21, transmit coil on port 1, receive coil on port 2 Spin echo images of water- filled phantom

Small surface coils with birdcage transmit coil Capacitively coupled coil with active detuning Inductively coupled coil with passive detuning Inductively coupled coil with active detuning Spin echo images of water-filled phantom SNR maps

Human finger joint images 1) 3D VIBE, res = 0.26 mm, sl th = 0.5 mm. 2) 3D FLASH, res = 0.20 mm, sl th = 0.3 mm. 3) TSE, res = 0.20 mm, sl th = 0.5 mm. 4) TOF3D, res = 0.20 mm, sl th = 1 mm

Ex vivo mouse brain at 3T 3D flash, in plane resolution 75  m, slice thickness 100  m, TR = 68 ms, TE = 13 ms, flip angle = 30°, 64 slices, 32 averages, total scan time = 9 hours

Conclusions Inductively coupled coils may be actively detuned by adding a third detuning coil controlled by pin diodes These coils are easy to construct and show no loss in SNR compared to coils using other methods of decoupling.

Acknowlegments Ray Nunnally, LCNI Scott Watrous, LCNI Cliff Dax, TSA, University of Oregon Felicia Katz, California Institute of Technology

Geometric decoupling Well aligned1° offset2° offset -45 dB-37 dB-31 dB

Geometric decoupling Place receive coil orthogonal to transmit RF field Advantages: conceptually simple, no additional components needed Disadvantages: Alignment must be precise