16:30 |
0142.
|
Measurement and
pre-emphasis of shim responses using frequency sweeps
Signe Johanna Vannesjo1, Benjamin Dietrich1,
Christoph Barmet1, Bertram J Wilm1,
David O Brunner1, and Klaas P Pruessmann1
1Institute for Biomedical Engineering,
University and ETH Zurich, Zurich, Switzerland
Dynamic use of higher-order shims to improve static B0,
puts increasing demands on characterization of shim
field dynamics and requires pre-emphasis implementations
to counteract eddy current effects. Measurements of the
shim impulse response function (SIRF), using a dynamic
field camera, and rectangular test functions, have
previously been shown to provide detailed information on
shim responses. Here, frequency-sweeped test pulses are
implemented for wide bandwidth coverage and increased
sensitivity of the SIRF measurements. It is shown that
SIRFs thus measured could form a basis for digital
pre-emphasis, enabling a flat frequency response and
fast shim settling after a switching event.
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16:42 |
0143.
|
Real-time shim
compensation in the human breast
Vincent Oltman Boer1, Mariska P. Luttje1,
Alex A. Bhogal1, Giel Mens2, Hans
Hoogduin1, Peter R. Luijten1, and
Dennis W.J. Klomp1
1Radiology, UMC Utrecht, Utrecht, Utrecht,
Netherlands, 2Philips
Medical Solutions, Best, Netherlands
Real-time control of the shim fields will allow for
compensation of B0 field
variations in the human body caused by breathing,
cardiac pulsation, non-voluntarily motion, scanner drift
etc. In this work the feasibility of real-time
measurement and updating of the shim fields is examined
and applied to real-time measurement and correction of
the B0 field
in the human breast at 7T.
|
16:54 |
0144. |
Measurement of microscopic
head motion during brain imaging
Julian Maclaren1, Brian S. Armstrong2,
Robb T. Barrows2, K. A. Danishad3,
Thomas Ernst4, Colin L. Foster2,
Kazim Gumus4, Michael Herbst1,
Ilja Y. Kadashevich3, Todd P. Kusik2,
Qiaotian Li2, Cris Lovell-Smith1,
Tom Prieto5, Peter Schulze3,
Oliver Speck3, Daniel Stucht3, and
Maxim Zaitsev1
1Dept. of Radiology, University Medical
Center, Freiburg, Germany, 2Electrical
Engineering, University of Wisconsin-Milwaukee, 3Biomedical
Magnetic Resonance, Otto-von-Guericke University,
Magdeburg, 4Dept.
of Medicine, University of Hawaii, 5Dept.
of Neurology, Medical College of Wisconsin
This work describes the design, construction and testing
of an MR-compatible in-bore camera capable of measuring
head motion with a precision of around 10 micrometres.
The system is used to quantify cardiac and
breathing-related head motion in normal subjects during
simultaneous MR imaging.
|
17:06 |
0145.
|
Reference Layer Artefact
Subtraction (RLAS): A novel method of minimizing EEG
artefacts during simultaneous fMRI.
Muhammad E.H. Chowdhury1, Karen J Mullinger1,
and Richard W Bowtell1
1SPMMRC, School of Physics and Astronomy,
University of Nottingham, Nottingham, Nottinghamshire,
United Kingdom
Large artefacts due to switched gradients, cardiac
pulsation and head movement compromise EEG data quality
during simultaneous EEG-fMRI. Artefacts are often
corrected using average artefact subtraction (AAS), but
small movements significantly hinder the performance of
AAS. Here we attenuate the artefacts by subtracting the
signal from a reference layer, which has a similar
conductivity to tissue and carries a set of electrodes
and leads that precisely overlay those attached to the
scalp. In experiments on a phantom and human subject
undergoing small movements, we demonstrate that
Reference Layer Artefact Subtraction (RLAS) outperforms
AAS in reduction of gradient and movement artefacts.
|
17:18 |
0146.
|
Discrete RF Coil
Components Introduce Significant Noise and Artifacts into
PET Images in Combined PET-MRI Systems
Geron A. Bindseil1, William B. Handler1,
and Blaine A. Chronik1,2
1Department of Physics and Astronomy,
University of Western Ontario, London, Ontario, Canada, 2Robarts
Research Institute, University of Western Ontario,
London, Ontario, Canada
In simultaneous PET-MRI, the RF coil is located within
the PET ring. Many RF coils consist of a symmetrical
arrangement of discrete highly attenuating components:
solder and capacitors. The authors investigated the
effect of a birdcage RF coil on PET image artifacts and
noise through a comprehensive Monte Carlo simulation
utilizing the commercial reconstruction software of the
small-animal system modeled. Attenuation-corrected PET
images from simulations with and without an RF coil were
compared. The RF coil case had 40% higher scatter
fraction, 25% higher noise and artifacts. RF coils
having discrete components in the PET FOV should be
designed carefully.
|
17:30 |
0147. |
MR-based Compensation of
Respiratory Motion Artifacts of In-Vivo PET Images Acquired
on a Simultaneous Whole-Body MR/PET System
Christian Würslin1, Holger Schmidt1,2,
Petros Martirosian1, Lars Stegger3,
and Nina Schwenzer1
1Dept. of Diagnostic and Interventional
Radiology, University Hospital Tübingen, D-72076
Tübingen, Germany, 2Department
of Preclinical Imaging and Radiopharmacy, University
Hospital Tübingen, Tübingen, Germany, 3Clinic
und Polyclinic of Nuklear Medicine, University Hospital
Münster, Münster, Germany
To compensate for respiratory motion artefacts in PET
images while maintaining full SNR using simultaneously
acquired MR images. Three patients underwent
simultaneous thoracic/abdominal PET/MR examination. PET
data were acquired in listmode. Simultaneous MR
acquisition yielded navigator data and 2D-multislice
data (each slice acquired 12x). Slices were sorted into
consistent blocks of anatomic information at different
respiratory states. Blocks were co-registered using
non-rigid registration yielding respiration-induced
tissue deformation fields. PET data were gated and
reconstructed. Then, PET images were aligned using the
deformation fields and summed up to obtain the final
images. Corrected PET images showed sharper edges at
similar SNR.
|
17:42 |
0148. |
Integrated 7T MRI and
SPECT Systems for Small-Animal Imaging
Mark Jason Hamamura1, Seunghoon Ha1,
Werner W Roeck1, James Hugg2, Dirk
Meier3, Bradley E Patt2, and Orhan
Nalcioglu1,4
1Tu & Yuen Center for Functional Onco-Imaging,
University of California, Irvine, CA, United States, 2Gamma
Medica, Inc., Northridge, CA, United States,3Gamma
Medica, Inc., Fornebu, Norway, 4Department
of Cogno-Mechatronics Engineering, Pusan National
University, Pusan, Korea, Republic of
The integration of small-bore MRI and SPECT systems for
back-to-back multimodality imaging has previously been
limited to magnetic field strengths of only 0.1 T.
Through the use of CZT-based nuclear radiation
detectors, we have integrated SPECT with a 7 T MRI
system for small-animal imaging. Co-registered MR and
SPECT images of a mouse injected with 99mTc
were acquired using this combined system.
|
17:54 |
0149.
|
Hybrid magnetic resonance
and ultrasound (MR-US) imaging as a novel method of High
Intensity Focused Ultrasound treatment guidance and
monitoring
Victoria Bull1, John Civale1, Ian
Rivens1, David J Collins2, Gail
ter Haar1, and Martin O Leach2
1Department of Radiotherapy and Imaging,
Institute of Cancer Research and Royal Marsden NHS
Foundation Trust, Sutton, Surrey, United Kingdom, 2CR-UK
and EPSRC Cancer Imaging Centre, Institute of Cancer
Research and Royal Marsden NHS Foundation Trust, Sutton,
Surrey, United Kingdom
Although MRI is considered the gold standard for HIFU
treatment guidance, it lacks the ability to interrogate
blood flow and monitor cavitation during treatments. A
hybrid MR-ultrasound (MR-US) imaging system has shown
promise as an improved technique, allowing real-time
Doppler ultrasound and B-mode cavitation detection to be
performed simultaneously with MR thermometry. A
comparative study of truly simultaneous MR-US
thermometry has also been conducted, showing good
correlation between measurements of temperature change.
The appearance of cavitation correlated with
fluctuations in MR thermometry, and colour Doppler added
dynamic information to MR angiographs. This system is a
strong candidate for clinical use.
|
18:06 |
0150.
|
MRI with Sideband
Excitation: Application to Continuous SWIFT
David O. Brunner1, Benjamin E. Dietrich1,
Matteo Pavan1, and Klaas P. Pruessmann1
1Institute for Biomedical Engineering,
University and ETH Zurich, Zurich, Zurich, Switzerland
Concurrent RF transmission and reception would be
beneficial for many applications in NMR such as imaging
of short T2-samples. Since the isolation
achieved by decoupling of transmit and receive paths is
typically not sufficient neither robust, the sideband
excitation approach is applied to isolate the excitation
pulse from the retrieved data. In conjunction with a
custom excitation chain and spectrometer, images have
been acquired using the SWIFT sequence with continuous
excitation and reception. RF transmitter infidelities
are captured by a real-time monitoring of the RF chain
allowing reconstructing the data on the excitation pulse
as measured in the coil.
|
18:18 |
0151.
|
Bloch Simulation of Human
MR Imaging at 14T
Zhipeng Cao1, Giuseppe Carluccio2,
Joshua Park3, Sukhoon Oh4, Zhang-Hee
Cho3, and Christopher M. Collins4
1Bioengineering, Penn State University,
Hershey, PA, United States, 2Electrical
Engineering, The University of Illinois at Chicago,
Chicago, IL, United States,3Neuroscience
Research Institute, Gachon University of Medicine and
Science, Incheon, Korea, Republic of, 4Radiology,
Penn State University, Hershey, PA, United States
The feasibility of human head imaging at 14T is explored
using a Bloch-based MRI simulator that considers
realistic B0, B1, and E1 distributions, including
multiple transmit and receive channels. Field
inhomogeneity, image SNR and SAR in the human head with
and without RF shimming are examined at 3T, 7T, and 14T.
The results showed a dramatic increase of image SNR from
3T to 14T, with a more subtle SAR increase, especially
from 7T to 14T.
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