|
Computer # |
|
3284.
|
49 |
Continuous Monitoring of
Radiofrequency Ablation using MR-based Fast Conductivity
Imaging Method
Woo Chul Jeong1, Saurav ZK Sajib1,
Ji Eun Kim1, Hyung Joong Kim1, Oh
In Kwon2, and Eung Je Woo1
1Kyung Hee University, Yongin, Gyeonggi,
Korea, 2Konkuk
University, Seoul, Korea
Estimation of ablated lesion and control of RF power is
important to reduce local recurrence after RF ablation,
there still exist needs for new bio-imaging technique
providing a non-invasive monitoring of RF ablation. We
proposed MR-based fast conductivity imaging for
monitoring of RF ablation using biological tissues. Fast
MREIT produces conductivity images at every 10.24
seconds during RF ablation. We could extract
spatiotemporal maps of tissue conductivity from a time
series of 180 conductivity images for 30.72 minutes.
Analyzing the time series of conductivity images, we
could distinguish six different stages and separately
interpret temperature-dependent and/or
structure-dependent conductivity changes.
|
3285.
|
50 |
Simultaneous Dual-frequency
Range Conductivity Mapping MR Method for Tissue
Characterization: In Vivo Canine Brain Disease Model Study
Woo Chul Jeong1, Min Oh Kim2,
Saurav ZK Sajib1, Ji Eun Kim1,
Hyung Joong Kim1, Oh In Kwon3,
Dong Hyun Kim2, and Eung Je Woo1
1Kyung Hee University, Yongin, Gyeonggi,
Korea, 2Yonsei
University, Seoul, Korea, 3Konkuk
University, Seoul, Korea
Electrical tissue conductivity is primarily determined
by concentration and mobility of ions in intra- and
extra-cellular fluids. The conductivity of biological
tissues show frequency-dependent behavior and its values
at different frequencies may provide useful diagnostic
information. MR-based tissue property mapping are widely
used imaging techniques which provided unique
conductivity contrast at different frequency ranges.
Recently, new method for data acquisition and
reconstruction for low- and high-frequency conductivity
images from a single MR scan was proposed. In this
study, we applied the simultaneous dual-frequency range
conductivity mapping to enhance its clinical potentials
through in vivo disease model animal imaging.
|
3286. |
51 |
Simultaneous Quantitative
Imaging method for Neuroimaging
Sung-Min Gho1, Jaewook Shin1,
Min-Oh Kim1, Dongyeob Han1, and
Dong-Hyun Kim1
1Electrical and Electronic Engineering,
Yonsei University, Sinchon-dong, Seoul, Korea
MR imaging can provide various quantitative information
regarding the electro-magnetic properties and relaxation
properties of tissue. The electric and magnetic
properties are linked through Maxwell's equations and
the magnetic susceptibility is one major source of the
R2* and R2'. These quantitative information can be used
independently, however, studies which use several
related quantitative information together can be useful
since mis-registration, different physiological noise
and lengthened scan time can be alleviated due to
separate measurements. In this abstract, we propose a
new method for obtaining these quantitative applications
simultaneously. Therefore, quantitative conductivity
map, QSM, R2*, and R2' maps.
|
3287. |
52 |
Electrical Conductivity
Images of Brain Metabolites using MR-based Tissue Property
Mapping
Saurav ZK Sajib1, Ji Eun Kim1, Woo
Chul Jeong1, Hyung Joong Kim1, Oh
In Kwon2, and Eung Je Woo1
1Kyung Hee University, Yongin, Gyeonggi,
Korea, 2Konkuk
University, Seoul, Korea
Electrical tissue conductivity is primarily determined
by concentration and mobility of ions. If electrical
current is carried by dissolved ions, the more ions
generate more currents. In addition, the mobility of
ions is restricted by heterogeneous membrane, current
density of tissue dependent on the physical environment
even though it has uniform ion concentration. Using
MREIT technique, we provide electrical
conductivity-based metabolite mapping with highly
sensitive to its concentration changes. Together with in
vitro measurement of metabolites by concentration
changes, we performed phantom imaging to evaluate the
proposed method showing a significant relationship
between concentration and electrical conductivity of
brain metabolites.
|
3288. |
53 |
Current-Controlled
Alternating Reversed DESS MREIT for Joint Estimation of
Tissue Relaxation and Electrical Properties
Hyunyeol Lee1 and
Jaeseok Park2
1Center for Neuroscience Imaging Research,
Institute for Basic Science (IBS), Sungkyunkwan
University, Suwon, Gyeonggi, Korea, 2Department
of Global Biomedical Engineering, Sungkyunkwan
University, Suwon, Gyeonggi, Korea
Conventional MREIT suffers from long imaging time and
low phase sensitivity, potentially resulting in
inefficient conductivity estimation. Current-controlled
alternating SSFP-FID was proposed as an alternative to
achieve rapid encoding as well as high nonlinear phase
sensitivity. Nevertheless, since the nonlinear phase
model includes both tissue relaxation and Bz properties,
the former has to be known as a priori for conductivity
estimation, which requires multiple separate
acquisitions. In this work, we propose a novel,
current-controlled alternating reversed dual echo steady
state (DESS) MREIT for joint estimation of tissue
relaxation and electrical properties in a single
measurement.
|
3289. |
54 |
GEOMETRICAL SHIFT RESULTS
IN ERRONEOUS APPEARANCE OF LOW FREQUENCY TISSUE EDDY CURRENT
INDUCED PHASE MAPS: THEORY, SIMULATIONS AND MEASUREMENTS
S. Mandija1, A.L.H.M.W. van Lier1,
P. Petrov2, S.W.F. Neggers2, P.R.
Luijten1, and C.A.T. van den Berg1
1Imaging Division, UMC Utrecht, Utrecht,
Netherlands, 2Brain
Center Rudolf Magnus, UMC Utrecht, Utrecht, Netherlands
In this abstract we demonstrate that combinations of
phase maps obtained with different gradient polarities
should be done carefully since these images are prone to
geometrical shift leading to RF phase falsely attributed
to LF phase. Since the RF phase is related to
conductivity at MHz frequency, because of this
geometrical displacement it appears that the LF phase is
also proportional to electrical conductivity. Instead,
as shown in simulations, if corrections are performed,
the LF phase is not measurable anymore, thus the scaling
of the LF phase with the conductivity can be attributed
to the RF phase leakage.
|
3290. |
55 |
Simulating Charge at
Electrical Property Interfaces
Eric Duggan Gibbs1,2 and
Chunlei Liu2,3
1Biomedical Engineering, Duke University,
Durham, NC, United States, 2Duke
University Medical Center, Brain Imaging and Analysis
Center, Durham, NC, United States, 3Department
of Radiology, Duke University, Durham, NC, United States
Eddy-currents generated by rapidly varying gradients
have been proposed as a current source to map electrical
properties of tissue non-invasively at low frequencies.
It has been suggested that charge accumulated at
electrical property interfaces potentially impacts the
recorded MR signal. Induced charges also may impact
images with conductive prosthetics. This work outlines
and demonstrates an algorithm that determines
electromagnetic fields in non-homogeneous materials and
accounts for charge accumulation due to eddy-currents
induced by rapidly varying gradients.
|
3291. |
56 |
Further Study of the
Effects of a Time-Varying Gradient Fields on Phase Maps –
Theory and Experiments
Jiasheng Su1, Bingwen Zheng2, Sam
Fong Yau Li2, and Shao Ying Huang1
1Singapore University of Technology and
Design, Singapore, Singapore, 2Department
of Chemistry, National University of Singapore,
Singapore
The method of retrieving conductivities of human tissues
through eddy currents induced by pulsed field gradient
was proposed and has been studied intensively. In this
abstract, an optimized electromagnetic (EM) model is
proposed to study the relation among encoding gradient
fields, the induced eddy currents, and the resultant
phase difference that was used for the retrieval of
conductivity. It is further applied to study the
relationship of the gradient fields, the pulse sequence,
and the resultant phase difference. Besides the
discharging process when the gradient field is a
constant that was identified previously, another crucial
discharging process to generate phase difference is
identified. This discharging process offset the phase
difference generated by that when gradient field is
constant. It is terminated when an RF pulse is applied.
This process is critical for obtaining meaningful phase
maps for the retrievals of conductivity. Both
theoretical and experimental results are presented.
|
3292. |
57 |
Water-Content-Map Assisted
Electrical Properties Reconstruction of Brain Tissue at 3T
Eric Michel1, Daniel Hernandez1,
Min Hyoung Cho1, and Soo Yeol Lee1
1Kyung Hee University, Suwon, Gyeonggi-Do,
Korea
Measuring the electrical properties of tissue
non-invasively with high resolution and accuracy has
practical significance for several diagnostic and
therapeutic applications in the biomedical field. In
this work, the relationship between the electrical
properties of tissue and their amount of electrolyte
content is exploited. This model is a combination of
previous observations of mixture theory and experimental
measurements given by literature. We validate our
formulation by performing in-vivo EPT mapping of brain
tissue at 3T MRI. Great accuracy with not precedent
resolution was achieved and we believe this method can
have a great impact in EPT estimations.
|
3293. |
58 |
In vivo reconstructed
conductivity values of cervical cancer patients based on EPT
at 3T MRI
Edmond Balidemaj1, Peter de Boer1,
Hans Crezee1, Rob Remis2, Lukas
Stalpers1, Aart Nederveen3, and
Cornelis A.T. van den Berg4
1Radiotherapy, Academic Medical Center,
Amsterdam, Netherlands, 2Circuits
and Systems Group, TU Delft, Delft, Netherlands, 3Radiology,
Academic Medical Center, Amsterdam, Netherlands, 4Radiotherapy,
UMC Utrecht, Utrecht, Netherlands
In this work we present in vivo reconstructed
conductivity values of cervical cancer patients using
Electric Properties Tomography (EPT) based on B1+ at 3T.
Conductivity values of muscle, bladder and cervical
tumors are presented. The results demonstrate the
importance of accounting for conductivity values in
living conditions when incorporating electric properties
data into numerical models.
|
3294. |
59 |
Effect of Ion Size on
Conductivity Measurements of MR-phase-based Electric
Properties Tomography.
Jan Sedlacik1, Ulrich Katscher2,
and Jens Fiehler1
1University Medical Center Hamburg-Eppendorf,
Hamburg, Hamburg, Germany, 2Philips
Research Europe, Hamburg, Germany
MR-based Electric Properties Tomography (EPT) provides a
non-invasive means to assess electric tissue properties
such as conductivity. EPT was shown to depend on ion
concentration and temperature. In this study the effect
of ion size, and therefore ion mobility, was studied.
The EPT-conductivity steeply changed between HCl and
NaOH which is caused by the much smaller free protons of
HCl as compared to NaOH. On the other side, the
contribution of the much larger glutamate ion on
EPT-conductivity is negligible, effectively bisecting
the amount of EPT-detectable ions and resulting in
nearly half conductivity of MSG as compared to NaCl.
|
3295. |
60 |
A Regularized Model-Based
Approach to Phase-Based Conductivity Mapping
Kathleen M Ropella1 and
Douglas C Noll1
1Biomedical Engineering, University of
Michigan, Ann Arbor, MI, United States
Phase-based conductivity mapping makes use of a noise
amplifying operation and often relies on spatial
filtering to reduce noise. This work describes a
regularized, model-based approach to conductivity
mapping, which is more robust in the presence of noisy
phase maps and provides better reconstruction near
boundaries. We demonstrate the efficacy of the algorithm
in simulations as well as in the human brain at 3.0T.
This method provides higher SNR and lower RMSE for
reconstructed conductivity maps as compared to a basic
spatial filtering approach.
|
3296. |
61 |
On the Signal-to-Noise
Ratio of MR-Based Electrical Properties Tomography
Seung-Kyun Lee1, Selaka Bandara Bulumulla1,
and Ileana Hancu1
1GE Global Research, Niskayuna, NY, United
States
We present calculation of the random noise-limited
signal-to-noise ratio (SNR) in MR-based electrical
properties tomography (MREPT). We find that the SNR in
the relative permittivity and electrical conductivity is
determined primarily by the SNR of the magnitude and the
phase of the B1+ map, respectively. In addition, the SNR
is proportional to the square of the linear dimension of
the region-of-interest, to the square root of the number
of voxels, and to the inverse square of the RF length
scales in the medium. Our results can inform design of
MREPT experiments with a desired SNR.
|
3297. |
62 |
Local Electrical Properties
Tomography With Global Regularization By Gradient
Jiaen Liu1, Xiaotong Zhang1, Yicun
Wang1, Pierre-Francois Van de Moortele2,
and Bin He1,3
1Biomedical Engineering, University of
Minnesota, Minneapolis, Minnesota, United States, 2Center
for Magnetic Resonance Research, University of
Minnesota, Minneapolis, Minnesota, United States, 3Institute
for Engineering in Medicine, University of Minnesota,
Minneapolis, Minnesota, United States
The in vivo electrical conductivity and permittivity of
tissues at Larmor frequency carries important
information for both diagnostic purpose and real-time
subject-specific local SAR quantification. Traditional
electrical properties tomography (EPT) derives a local
solution and can be severely deteriorated due to noise
contamination. In the present study, a new approach was
proposed to improve the local EPT solution with global
regularization by the spatial gradient information of
electrical properties, which is deducted from measured
transmit B1 field induced in a multi-channel
radiofrequency coil. Experiments involving a controlled
physical phantom and healthy human subject were
conducted to evaluate the proposed algorithm.
|
3298. |
63 |
Combination of multichannel
receive data for local cr-MREPT
Necip Gurler1, Omer Faruk Oran1,
and Yusuf Ziya Ider1
1Department of Electrical and Electronics
Engineering, Bilkent University, Ankara, Turkey
Convection-reaction equation based MREPT (cr-MREPT) is
known to reconstruct electrical properties (EPs) also in
transition regions where EPs vary. However it results in
artifacts in regions where “the convective field” is
low. Use of multichannel receive data with different and
possibly non-overlapping low convective field regions
provides the opportunity for artifact free
reconstruction of EPs. In this study, a method is
developed for combining multichannel receive data to
image EPs in a “local region of interest”. The method
has been successfully applied in both phantom and
healthy human brain experiments.
|
3299. |
64 |
Low pass filter based
electrical property tomography (EPT) reconstruction
Jaewook Shin1, Min-oh Kim1, Narae
Choi1, and Dong-Hyun Kim1
1Electrical and Electronic Engineering,
Yonsei University, Seodaemun-gu, Seoul, Korea
Magnetic resonance electrical properties tomography
(MREPT) is currently being investigated for many
clinical applications. However, MREPT suffers from
statistical noise and boundary artifact. Especially, the
noise amplification in MREPT is occurred due to the
calculation of the Laplacian operator. To overcome this
EPT error, filtering or fitting based technique was
introduced. In this study, low pass filter (LPF) based
EPT reconstruction method without the Laplacian operator
is proposed.
|
3300. |
65 |
PDE Solution of Electrical
Properties Tomography With Multi-channel B1 Transmission
Jiaen Liu1, Yicun Wang1, Xiaotong
Zhang1, Pierre-Francois Van de Moortele2,
and Bin He1,3
1Biomedical Engineering, University of
Minnesota, Minneapolis, Minnesota, United States, 2Center
for Magnetic Resonance Research, University of
Minnesota, Minneapolis, Minnesota, United States, 3Institute
for Engineering in Medicine, University of Minnesota,
Minneapolis, Minnesota, United States
Electrical properties tomography (EPT) is recently
introduced for imaging the electrical properties of
tissue using MRI. The EPT equation can be transformed
into a partial different equation (PDE) and solved using
numerical PDE solutions. The advantage of the PDE-based
approach is improved EP result near the boundary and
enhanced robustness against noise contamination. A
multi-channel transceiver RF coil was utilized to
provide multiple transmit B1 field for solving the PDE.
The method does not require assumption of equal transmit
and receive RF phase, and eliminates the need of
pre-assigned boundary condition by using multiple
excitations, beneficial for in vivo applications.
|
3301. |
66 |
Minimum-noise Laplacian
kernel for MR-based electrical properties tomography
Seung-Kyun Lee1
1GE Global Research, Niskayuna, NY, United
States
Noise amplification by Laplacian operation on a noisy
input RF map is an important limiting factor in the SNR
of MR-based electrical properties tomography (MREPT). We
show that among all linear Laplacian kernels, the one
based on the Savitzky-Golay second-order derivative
kernel has the least amount of noise amplification. A
method to construct such a kernel for an arbitrary
three-dimensional ROI is presented, and its performance
is compared with other Laplacian kernels used in
literature.
|
3302. |
67 |
The dielectric properties
of brain tissues: variation in electrical conductivity with
tissue sodium concentration and tissue water content at
3T/4T
YuPeng Liao1, Sandro Romanzetti1,
Vincent Gras1, DengFeng Huang1,
and N. Jon Shah1,2
1Institute of Neuroscience and Medicine-4,
Forschungszentrum Juelich, Juelich, Germany, 2JARA-Faculty
of Medicine, RWTH Aachen University, Aachen, Germany
MRI can be used to non-invasively estimate in vivo
electrical conductivity, tissue water content, tissue
sodium content (TSC) . In this study we compare proton
density (PD), TSC and conductivity distributions in
healthy volunteers. This combined study of the three
maps, conductivity, PD, and TSC for the first time,
allows us to describe the contribution of the tissue
water contents and tissue ion concentration (Na+) to the
tissue conductivity data and empirical relationship
models may be used to predict dielectric properties in
other frequency and tissues.
|
3303. |
68 |
Total Variance Constrained
Electrical Properties Tomography Using a 16-channel
Transceiver Array Coil at 7T
Yicun Wang1, Xiaotong Zhang1,
Jiaen Liu1, Pierre-Francois Van de Moortele2,
and Bin He1,3
1Department of Biomedical Engineering,
University of Minnesota, Minneapolis, Minnesota, United
States, 2Center
for Magnetic Resonance Research, University of
Minnesota, Minneapolis, Minnesota, United States, 3Institute
for Engineering in Medicine, University of Minnesota,
Minneapolis, Minnesota, United States
Electrical Properties Tomography (EPT) is able to
provide quantitative maps of electrical properties (EP)
using MRI, which holds promise in early cancer
diagnosis. Currently, the Helmholtz Equation-based EPT
approaches ignore gradient information on the tissue
boundary, causing severe EP reconstruction artifacts;
other studies require either a priori boundary
conditions that are subject to error, or dielectrical
padding that may cause difficulties in practical
settings. In this study, we proposed a total variance
promoting gradient-based algorithm that does not bear
the aforementioned limitations. Simulation and phantom
experiment at 7T have demonstrated feasibility of this
new approach.
|
3304. |
69 |
Calculation of
Electromagnetic Field Distribution to Detect Liver
Abnormalities using MR-based Electrical Impedance Tomography
Ji Eun Kim1, Saurav ZK Sajib1, Woo
Chul Jeong1, Hyung Joong Kim1, Oh
In Kwon2, and Eung Je Woo1
1Kyung Hee University, Yongin, Gyeonggi,
Korea, 2Konkuk
University, Seoul, Korea
Electromagnetic field distribution of biological system
can be imaged from magnetic flux density which was
induced by externally injected current through the
electrodes. Electromagnetic field is affected by
injected current and electrical conductivity of tissues,
electrode type and position are important factors for
determining voltage and current density. Signal
intensity of current density is proportional to magnetic
flux density which can be measured by MREIT. MREIT has
potential to provide high-resolution electromagnetic
field distribution inside the liver. Using a
three-dimensional FEM model, we estimate current pathway
and electrical field distribution to detect liver
abnormalities at three different current injection
methods.
|
3305. |
70 |
Anisotropic Conductivity
Distribution of Brain using a Combination of DTI and MREIT
Saurav ZK Sajib1, Woo Chul Jeong1,
Ji Eun Kim1, Hyung Joong Kim1, Oh
In Kwon2, and Eung Je Woo1
1Kyung Hee University, Yongin, Gyeonggi,
Korea, 2Konkuk
University, Seoul, Korea
Estimation of brain anisotropic conductivity has a
potential in analysis of interactions between
electromagnetic fields and biological systems, such as
prediction of current pathway in tDCS and DBS. In this
study, we reconstruct anisotropic conductivity
distribution of canine brain by combing information from
the DTI and MREIT imaging. Since the MREIT technique is
used for visualizing high-resolution isotropic
conductivity at low frequency. Combing the measured
water self-diffusion from DTI and z-component of
magnetic flux density from MREIT, it is possible to
obtain effective-conductivity-to-diffusivity ratio (ECDR)
in every voxels which provides precise information for
brain anisotropy comparing to global scaling factor.
|
3306. |
71 |
Investigating breast tumor
malignancy with electric conductivity measurement
Ulrich Katscher1, Hiroyuki Abe2,
Marko K Ivancevic3, and Jochen Keupp1
1Philips Research Europe, Hamburg, Germany, 2Medical
Center, University of Chicago, Chicago, Illinois, United
States, 3Philips
Healthcare, Best, Netherlands
According to ex vivo studies, breast tumors exhibit a
significantly altered conductivity, which opens the
chance to increase MRI specificity of breast tumor
characterization. Conductivity can be measured in vivo
using “Electric Properties Tomography” (EPT). With EPT,
a trend towards a correlation between conductivity and
malignancy was indicated in initial breast tumor
studies, however, without statistical significance. This
study tests a statistically significant correlation
between conductivity and malignancy. Lesion volume
derived from pre/post contrast subtraction images was
used as a priori information to stabilize EPT
reconstruction. According to the results obtained, EPT
is able for tumor malignancy staging.
|
3307. |
72 |
Correlation between the
electric conductivity measured by MREPT and apparent
diffusion coefficient in invasive breast cancer - permission withheld
Min Jung Kim1, Soo-Yeon Kim1,
Dong-Hyun Kim2, Jaewook Shin2, and
Eun-Kyung Kim1
1Yonsei University, Seoul, Korea, 2Yonsei
University, Korea
There is an inverse correlation between conductivity and
ADC in invasive breast cancer. Necrosis may have an
effect to increase conductivity since cell membranes
that are barriers for ionic movement are disrupted by
necrosis.
|
|
|
Computer # |
|
3308. |
73 |
COMbining Phased array data
using Offsets from a Short Echo-time Reference scan
(COMPOSER)
Simon Daniel Robinson1, Wolfgang Bogner1,
Barbara Dymerska1, Pedro Cardoso1,
Günther Grabner1, Xeni Deligianni2,
Oliver Bieri2, and Siegfried Trattnig1
1High Field MR Centre, Department of
Biomedical Imaging and Image-guided Therapy, Medical
University of Vienna, Vienna, Vienna, Austria, 2Division
of Radiological Physics, Department of Radiology,
University of Basel Hospital, Basel, Switzerland
We present a phase-sensitive method for the combination
of data from array coils for which there is no volume
reference coil, such as PTx and some UHF receive arrays.
A very fast variable echo-time (vTE) reference scan with
a sub-millisecond TE is used to measure the complex
sensitivity of the array. Dividing high resolution,
T2*-weighted (e.g. SWI) data by the vTE scan matches the
phase of the array elements, allowing the complex
signals to be combined. This approach is fast, robust,
requires no phase unwrapping of phase and outperforms
the rival methods tested.
|
3309. |
74 |
Multi-channel data
combination with linear phase baseline correction
Saifeng Liu1, Yongquan Ye2, Sagar
Buch3, and E. Mark Haacke1,2
1The MRI Institute for Biomedical Research,
Waterloo, Ontario, Canada, 2Department
of Radiology, Wayne State University, Detroit, Michigan,
United States,3School of Biomedical
Engineering, McMaster University, Hamilton, Ontario,
Canada
When GRAPPA is used for parallel imaging, magnitude and
phase images will be reconstructed for each channel of
the array coil before being combined for the final
images. Simple weighted averaging of the complex data
may lead to a particular singularity artifact in phase
images, attributed to the variation in the baseline
phase components (φ0) between different channels. In
this study, we propose an algorithm in which the coil
sensitivity induced phase component is modelled as 3D
linear function, and can be corrected effectively in
k-space domain.
|
3310. |
75 |
Multi-Echo Multi-Receiver
MR Phase Reconstruction with Bipolar Acquisitions
Joseph Dagher1
1Department of Medical Imaging, University of
Arizona, Tucson, AZ, United States
Multi-Echo Gradient Echo phase measurements are
important in various MR applications. Bipolar
acquisitions of the MEGE echoes in a given TR allow for
shorter inter-echo spacing and higher SNR efficiency
than monopolar acquisitions, but introduce an unknown
spatially varying phase between even and odd echoes. We
propose here a strategy for reconstructing the
underlying phase, as acquired with an array of receive
coils using bipolar echoes, without requiring a
reference scan. Our method separates the phase due to
the underlying physiology from the phase offsets of the
receive coils and the even-odd echoes, using a unifying
Maximum-Likelihood framework.
|
3311. |
76 |
The impact of background
removal techniques on the quantification of magnetic
susceptibility in the human cortex
Diana Khabipova1 and
José P. Marques1
1CIBM, Lausanne, Vaud, Switzerland
Quantitative susceptibility mapping (QSM) is sensitive
to iron and myelin but pre-processing need to be
performed in order to retrieve the QSM maps. The
background removal step was analyzed and the performance
and quality of some of the state of art background
removal techniques in the estimated susceptibility of
the brain cortex was compared in this study for the
first time. While all methods have the expected high
susceptibility values of primary sensory areas in the
layer close to the white matter, the main differences
lay in the outer layer of the brain cortex.
|
3312. |
77 |
DirEct Complex signAl
Fitting (DECAF) for multi-compartment analysis in white
matter
Yoonho Nam1, Dong-Hyun Kim2, and
Jongho Lee1
1Department of Electrical and Computer
Engineering, Seoul National University, Seoul, Seoul,
Korea, 2Department
of Electrical and Electronic Engineering, Yonsei
University, Seoul, Korea
Recent studies have demonstrated that signals from three
water compartments in white matter have different B0
orientation dependent frequency offsets. This
observation improved data fitting results in GRE-based
MWI by using complex signal fitting as compared to
magnitude signal fitting. However, the complex signal
fitting approaches applied in the previous studies
required several pre-processing steps including a
nonlocal background field removal step. Therefore, the
results were strongly influenced by them. In this study,
we propose a new fitting method that does not require a
prior background field removal step. This method shows
improvement in parameter estimation.
|
3313. |
78 |
iHARPERELLA: an improved
method for integrated 3D phase unwrapping and background
phase removal
Wei Li1,2, Bing Wu3, and Chunlei
Liu4,5
1Research Imaging Institute, University of
Texas Health Science Center at San Antonio, San Antonio,
TX, United States, 2Ophthalmology,
University of Texas Health Science Center at San
Antonio, San Antonio, TX, United States, 3GE
Healthcare, Beijing, China, 4Brain
Imaging and Analysis Center, Duke University, Durham,
NC, United States, 5Radiology,
Duke University, Durham, NC, United States
Quantitative susceptibility mapping requires reliable 3D
phase unwrapping and background phase removal.
Previously, we have developed a method for integrated 3D
phase unwrapping and harmonic background phase removal
using Laplacian, namely HARPERELLA. In this study, we
introduced an improved version of this HARPERELLA
method, which allows more intuitive implementation and
more robust suppression of the low frequency background
phase. Importantly, it also provides the selection
between smooth phase throughout the field of view or
intact local phase variations around the veins by
choosing between Laplacian-based and path-based phase
unwrapping.
|
3314. |
79 |
Quantitative Assessment of
Background Field Removal Methods for Abdominal Imaging
Debra E. Horng1,2, Samir D. Sharma1,
Diego Hernando1, and Scott B. Reeder1,2
1Radiology, University of Wisconsin-Madison,
Madison, WI, United States, 2Medical
Physics, University of Wisconsin-Madison, Madison, WI,
United States
Background field removal is a necessary step for
accurate QSM (susceptibility estimation). We assess the
performance of currently used background field removal
algorithms (PDF and SHARP), in the context of abdominal
imaging. Compared to brain iron, liver iron is spatially
diffuse, highly concentrated, and situated closer to
air. Large and small containers (6cm and 1.6 diameters)
containing gadolinium dilutions, positioned both close
and far from air, produced field maps; the dilutions
corresponded to susceptibilities of -7.3, -5.6, -3.9,
and -2.1 ppm. Both PDF and SHARP result in less than 0.6
Hz/voxel error in the local field estimate.
|
3315. |
80 |
Removal of Background
Fields with Spatially Variable Kernel Radii Guided by the
Frequency-Offset-Gradient (FOG) Magnitude
PINAR SENAY ÖZBAY1,2, Cristina Rossi1,
Klaas Paul Prüssmann2, and Daniel Nanz1
1Department of Radiology, University Hospital
Zürich, Zürich, Switzerland, 2Institute
of Biomedical Engineering, ETH Zürich, Zürich,
Switzerland
The calculation of quantitative susceptibility maps,
QSM, requires removal of non-local fields, e.g., via a
convolution of a phase map with a Laplacian-kernel,
multiplication with an eroded-binary-tissue-mask, and
deconvolution. While erosion of the tissue-mask improves
QSM image quality, valuable information is lost. The
goal of this study was to regionally vary the size of
the Laplacian convolution kernel based on the magnitude
of the Frequency-Offset-Gradient-(FOG), which tends to
be higher in regions close to the cavities, where
air-tissue-susceptibility-artifacts are severe.
Susceptibility-maps calculated with the variable-kernel
approach revealed less-artifact, and gave more realistic
information around the brain-tissue close to the
cavities.
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3316. |
81 |
regularized QSM with
instant parameter sweep and reduced streaking artifacts in
seconds
Job G. Bouwman1 and
Peter R Seevinck1
1Image Sciences Institute, University Medical
Center Utrecht, Utrecht, Netherlands
Instant parameter sweep for L2-regularized Quantitative
Susceptibility Mapping, combined with
efficient/automatic spatial buffer handling reducing
wrap-around streaking.
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3317. |
82 |
Quantitative Susceptibility
Mapping of Intracranial Hemorrhage: Artifacts Reduction
Hongfu Sun1, Mahesh Kate2, Laura
C. Gioia2, Derek J. Emery3,
Kenneth Butcher2, and Alan H. Wilman1
1Biomedical Engineering, University of
Alberta, Edmonton, AB, Canada, 2Neurology,
U of Alberta, AB, Canada, 3Radiology,
U of Alberta, AB, Canada
We propose a masking dipole inversion and superposition
QSM reconstruction method to reduce the artifacts
associated with intracranial hemorrhage, in cases of
standard susceptibility-weighted imaging using a single
long echo.
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3318. |
83 |
Streaking Artifacts
Reduction for QSM
Hongjiang Wei1, Wei Li2, Nian Wang1,
and Chunlei Liu1,3
1Brain Imaging and Analysis Center, Duke
University, Durham, NC, United States, 2University
of Texas Health Science Center at San Antonio, TX,
United States, 3Depatment
of Radoilogy, School of Medicine, Duke University,
Durham, NC, United States
Quantifying susceptibility from the phase image is
hampered by the ill-posed dipole filter inversion
problem. The imperfect inversion on and near the conical
surface results in streaking artifacts in the computed
susceptibility maps. In this study, we introduced a
novel image-space weighting function to suppress errors
induced by imperfect phase measurement and unwrapping.
This weighting function is applied in a joint L1 and L2
norm minimization procedure which can be solved rapidly
using SPARSA solver. A significantly lower level of
streaking artifacts is observed in the resulting
susceptibility maps. The results are comparable to those
obtained from COSMOS method, and the computation time
for the reconstruction is less than one minute for a
matrix size of 320×320×204
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3319. |
84 |
Quantitative Susceptibility
Mapping Using Adaptive Edge-Preserving Filtering
Toru Shirai1, Ryota Sato1, Yo
Taniguchi1, Takenori Murase2,
Yoshitaka Bito2, and Hisaaki Ochi1
1Central Research Laboratory, Hitachi, Ltd.,
Kokubunji, Tokyo, Japan, 2MRI
system division, Hitachi Medical Corporation, Chiba,
Japan
We propose a novel QSM reconstruction method that
reduces the artifacts and generates a high quantitative
susceptibility map without the regularization term. The
method consists of three steps: (I) iterative least
square minimization, (II) adaptive edge-preserving
filtering to the susceptibility map in the minimization
process, and (III) weighted addition of the
susceptibility map in k-space before and after
filtering. The results of a 3D numerical phantom
simulation and healthy volunteer experiment showed that
the method may be useful for reducing streaking
artifacts and generating a susceptibility map of which
quantitative is maintained.
|
3320. |
85 |
Enhancing K-Space Methods
for Quantitative Susceptibility Mapping by Exploiting
Consistency in Cone Data
Yan Wen1,2, Yi Wang2,3, and Tian
Liu1
1MedImageMetric LLC, New York, New York,
United States, 2Biomedical
Engineering, Cornell University, Ithaca, New York,
United States, 3Radiology,
Weill Cornell Medical College, New York, New York,
United States
K-space QSM algorithms are computationally inexpensive
and easy to implement. But their results usually
contains streaking artifacts. Here, we introduce a
method that can be applied to an existing k-space
results to improve its accuracy and suppress streaking
artifacts by constraining the energy of the data in the
cone region to the energy of the data in non-cone
region, and enforcing structure consistency with
sophisticated prior data. This post-QSM method was
tested on a gadolinium phantom and an in vivo human
brain, and it demonstrated the suppression of streaking
artifacts as well as the recovery of cone region data.
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3321. |
86 |
Quantitative Susceptibility
Mapping using Segmentation-Enabled Dipole Inversion
Jakob Meineke1, Julien Senegas1,
Ulrich Katscher1, and Fabian Wenzel1
1Philips Research Europe, Hamburg, Hamburg,
Germany
Quantitative Susceptibility Mapping is an ill-posed
problem that requires two computational steps:
background-field removal and dipole inversion. This work
focuses on QSM in the brain and describes susceptibility
reconstruction using reliable, a priori knowledge from
automated segmentation of anatomical ROIs. Background
field removal is integrated with dipole inversion in a
single-step minimization problem by computing the
sources of the magnetic field perturbation which is
generated by the tissue susceptibility. This method,
dubbed segmentation-enabled dipole inversion (SEDI),
results in a more accurate susceptibility
reconstruction.
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3322. |
87 |
Structural feature based
collaborative reconstruction for quantitative susceptibility
mapping
Lijun Bao1,2, Zhong Chen1, Peter
C.M. van Zijl2, and Xu Li2
1Department of Electronic Science, Xiamen
University, Xiamen, Fujian, China, 2Department
of Radiology,School of medicine, Johns Hopkins
University, Baltimore, MD, United States
Quantitative susceptibility mapping enables non-invasive
mapping and quantitative analysis of tissue
susceptibility. Interest in this methodology is
increasing, because it has the potential to facilitate
diagnosis of cerebrovascular and nervous system
diseases. However, the reconstruction of magnetic
susceptibility constants from local phase information is
an ill-posed inverse problem. Therefore, the development
of methods to reconstruct accurate susceptibility
distributions is important. We present a structural
feature based collaborative reconstruction method for
quantitative susceptibility mapping. Experimental
results on human brain show that this method can provide
high quality images of quantitative susceptibility and
improve the reconstruction accuracy.
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3323. |
88 |
Distribution Specified
Dipole Inversion for Quantitative Susceptibility Mapping
Yilin Yang1, Tian Liu2, Jianwu
Dong3, Pascal Spincemaille4, and
Yi Wang4,5
1Department of Electronic Engineering,
Tsinghua University, Beijing, Beijing, China, 2MedImageMetric,
LLC, New York, NY, United States, 3Department
of Automation, Tsinghua University, Beijing, Beijing,
China, 4Department
of Radiology, Weill Medical College of Cornell
University, New York, NY, United States,5Department
of Biomedical Engineering, Cornell University, Ithaca,
NY, United States
Dipole inversion is the final step of the QSM algorithm.
In this step, the zero cone surface in the dipole kernel
makes the field-to-susceptibility inverse problem
ill-posed. Current solutions are mostly based on the
Bayesian approach. Previous techniques have used
weighted L1-norm with binary weights derived from the
gradient echo magnitude image or phase image. Taking the
information from the distribution of the susceptibility
gradient into account could improve the reconstructed
image. And L2-norm converges faster than L1-norm.
Therefore, we employ reweighted L2-norm to specify the
distribution to Gaussian. The results of this novel
Distribution Specified Dipole Inversion (DSDI) method
demonstrate an enhancement of QSM reconstruction and a
significant shortening in calculation time.
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3324. |
89 |
Quantitative susceptibility
mapping using piecewise gradient weighting
Zhiwei Zheng1, Shuhui Cai1, Congbo
Cai2, and Zhong Chen1
1Department of Electronic Science, Xiamen
University, Xiamen, Fujian, China, 2Department
of Communication Engineering, Xiamen University, Xiamen,
Fujian, China
Quantitative susceptibility mapping has found many
promising research and clinical applications recently.
However, efficient reconstruction method of
susceptibility map remains necessary. We propose to
reconstruct susceptibility map using a piecewise
gradient from estimated susceptibility itself. The
gradually varied weighting is different from the
traditional binary weighting. Our method is compared to
morphology enabled dipole inversion (MEDI) method, and
the results indicate that our method has a better
performance in susceptibility reconstruction.
|
3325. |
90 |
Quantitative susceptibility
mapping with superfast dipole inversion: Influence of
regularization parameters on the susceptibility of the
substantia nigra and the red nucleus
Olaf Dietrich1, Seyed-Ahmad Ahmadi2,
Johannes Levin2, Juliana Maiostre2,
Annika Plate2, Armin Giese3, Kai
Bötzel2, Maximilian F Reiser1,4,
and Birgit Ertl-Wagner4
1Josef Lissner Laboratory for Biomedical
Imaging, Institute for Clinical Radiology, LMU Ludwig
Maximilian University of Munich, Munich, Germany, 2Department
of Neurology, LMU Ludwig Maximilian University of
Munich, Munich, Germany, 3Center
for Neuropathology and Prion Research, LMU Ludwig
Maximilian University of Munich, Munich, Germany, 4Institute
for Clinical Radiology, LMU Ludwig Maximilian University
of Munich, Munich, Germany
The purpose of this study was to analyze the influence
of the regularization parameters on the results of
quantitative susceptibility mapping using the superfast
dipole inversion (SDI) technique. SDI is performed in
the Fourier domain by multiplication with an SDI kernel,
which depends on two regularization parameters for the
regularization (1) of the Laplace operator inversion and
(2) of the unit dipole inversion (in the Fourier
domain). Both parameters were varied and the
susceptibility of the substantia nigra and the red
nucleus were assessed. The results showed a substantial
variation of the susceptibility depending on the
regularization.
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3326. |
91 |
On the feasibility of QSM
in MR-invisible regions
Diego Hernando1, Debra E. Horng1,2,
Samir D. Sharma1, and Scott B. Reeder1,2
1Radiology, University of Wisconsin-Madison,
Madison, WI, United States, 2Medical
Physics, University of Wisconsin-Madison, Madison, WI,
United States
QSM has the potential to probe MR-invisible objects,
based on the effect of their magnetic susceptibility on
the nearby B0 field in MR-visible regions. However, the
fundamental ability to map magnetic susceptibility of
MR-invisible objects based on nearby B0 measurements has
not yet been characterized. In this work, we address
this question with phantom experiments and singular
value decomposition analysis. Our results demonstrate
that susceptibility measurement may be feasible in
MR-invisible regions if the susceptibility distribution
can be assumed to be homogeneous over the MR-invisible
region of interest. However, susceptibility mapping of
spatially-varying susceptibility distributions in
MR-invisible regions is an inherently challenging
problem.
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3327. |
92 |
On the influence of zero
padding on the non linear operations of quantitative
susceptibility mapping
Sarah Eskreis-Winkler1, Dong Zhou2,
Tian Liu3, Ajay Gupta2, Susan
Gauthier2, Yi Wang2, and Pascal
Spincemaille2
1Weill Cornell Medical College, New York, NY,
United States, 2Weill
Cornell Medical College, New York, United States, 3MedImageMetric,
LLC, New York, United States
Zero padding is a well-studied interpolation technique
that improves image visualization without increasing
image resolution. Here, however, we demonstrate the
unique effect of performing zero padding in conjunction
with the nonlinear Quantitative Susceptibility Mapping
(QSM) algorithm. We assess the effects of this
combination by evaluating apparent spatial resolution,
relative error and depiction of multiple sclerosis (MS)
lesions on QSM.
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3328. |
93 |
p-space imaging: Where does
the contrast come from?
Sina Straub1, Andreas Wetscherek1,
Mark E. Ladd1, and Frederik B. Laun1
1Medical Physics in Radiology, German Cancer
Research Center (DKFZ), Heidelberg, Germany
The effect of p-space imaging is simulated for a voxel
filled with myelinated axons compared to a voxel with
homogeneous magnetization. P-space can be obtained by
sampling k-space with a standard gradient echo sequence
and applying additional gradients before the imaging
gradients. In the simulations, little to no difference
is observed between the MR signal of the voxel with
substructure and the one with homogeneous magnetization.
P-space MR experiments, however, showed partial volume
effects and signal enhancement in phase and magnitude
images that are indicative of subvoxel structure.
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3329. |
94 |
Compressed Sensing (CS) in
phase imaging requires dedicated reconstruction strategies
Ukash Nakarmi1, Shruti Prasad2,
Leslie Ying1,3, Paul Polak2,
Robert Zivadinov2,4, and Ferdinand Schweser2,4
1Dept. of Electrical Engineering, State
University of New York at Buffalo, Buffalo, NY, United
States, 2Buffalo
Neuroimaging Analysis Center, Dept of Neurology, School
of Medicine and Biomedical Sciences, State University of
New York at Buffalo, NY, United States, 3Dept.
of Biomedical Engineering, State University of New York
at Buffalo, NY, United States, 4MRI
Molecular and Translational Imaging Center, Buffalo
CTRC, State University of New York at Buffalo, Buffalo,
NY, United States
Application of conventional Compressive Sensing (CS)
paradigm on sparse signal reconstruction for
Quantitative Susceptibility Mapping is investigated.
Frontiers and limitations of CS reconstruction in
undersampled GRE data with long echo times and strong
phase, and its corresponding effects on tissue
characteristics and microstructures on reconstructed
images for QSM is investigated.
|
3330. |
95 |
Improved Accuracy in
Susceptibility-based OEF Measurements by Mitigation of
Partial-Volume Effects via Combined Magnitude and Phase
Reconstruction
Patrick McDaniel1, Audrey Fan2,
Berkin Bilgic3, Jeffrey N. Stout4,
and Elfar Adalsteinsson1,4
1Electrical Engineering and Computer Science,
Massachusetts Institute of Technology, Cambridge, MA,
United States, 2Radiology,
Richard M. Lucas Center for Imaging, Stanford
University, Stanford, CA, United States, 3A.
A. Martinos Center for Imaging, Department of Radiology,
Massachusetts General Hopsital, Charlestown, MA, United
States, 4Health
Sciences and Technology, Harvard-MIT, Cambridge, MA,
United States
Regional quantitative Oxygen Extraction Fraction (OEF)
values measured using MRI phase data are clinically
valuable, but can only be reliably obtained from blood
vessels larger than the acquisition voxel size. Blood
vessels beyond this limit produce unreliable
measurements because of partial-volume effects. We
demonstrate a method for obtaining more reliable OEF
measurements beyond this limit by amending the
conventional phase-based reconstruction with additional
information contained in the magnitude of the
complex-valued MR signal. The method is validated on
numerical and in vivo data over a range of voxel sizes
from ½ to 3 times the vessel diameter.
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3331.
|
96 |
On the limitations of brain
lesion characterization by direct assessment of MRI phase
Paul Polak1, Robert Zivadinov1,2,
and Ferdinand Schweser1,2
1Department of Neurology, Buffalo
Neuroimaging Analysis Center, State University of New
York at Buffalo, Buffalo, NY, United States, 2Molecular
and Translational Imaging Center, MRI Center, Clincal
and Translational Research Center, Buffalo, NY, United
States
Differentiation of hemorrhagic and calcified brain
lesions is an important clinical neuroimaging task. The
gold-standard technique uses computed tomography,
although the use of susceptibility weighted phase images
has been the subject of intense research. On the basis
that hemorrhages are paramagnetic, and calcifications
diamagnetic, the phase of the lesion can be used as the
criterion for differentiation. In numerical simulations
of an elliptical lesion we demonstrated that the
internal phase also depends on the lesion’s orientation
in the magnetic field, and thus phase is an unreliable
standard for lesion discrimination. Quantitative
susceptibility maps derived from the phase images
correctly recovered the underlying susceptibility
regardless of positioning, and thus are a better
differentiator of lesion subtypes.
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