Eddy Solomon1, Thomas Vahle2, Jan Paska1, Kai Tobias Block1, Daniel K. Sodickson1, Fernando Boada1, and Hersh Chandarana1
1Radiology, New York University School of Medicine, New York, NY, United States, 2Siemens Healthcare GmbH, Erlangen, Germany
Synopsis
The sensitivity of MRI sequences to
motion impairs their reliability and diagnostic utility for examining the chest
and abdomen. Established motion-compensation techniques are not accurate enough,
come at the cost of patient comfort, and are limited by the MR imaging
parameters. Here, we demonstrate a novel approach that detects respiratory
signal from the amplitude modulation of a transmitted RF reference signal,
termed ‘pilot-tone’ (PT). We show how the use of this simple RF transmitter,
with its small dimensions, high sampling rate, and low interference with the MR
acquisition, can produce motion corrected-images under free-breathing
conditions.
INTRODUCTION
The slow acquisition speed of MRI can limit
its applicability for examination of the chest and abdomen, often leading to motion
artifacts caused by physiological movements such as cardiac and respiratory
motion (1). External sensors (2) such as respiratory belts have
traditionally been used for triggering the acquisition. However, this approach is
oftentimes unreliable and tends to suffer from poor sensitivity. Self-navigation (3), on the other hand, extract motion information
from k-space center, which introduces a dependency on imaging parameters (e.g. TR,
number of slices) and can be too slow for certain types of physiological motion.
In this work, we demonstrate an alternative approach which provides
respiratory information with high temporal resolution. A reference RF signal (4), termed “pilot tone”
(PT), is generated by a small radiofrequency transmitter and received by the MR
system during each readout. Because the PT amplitude is modulated by the
subject’s breathing pattern, a respiratory signal can be derived. The PT approach
was tested using a radial MR sequence on human volunteers, and was compared to conventional
methods for motion correction. METHODS
Experiment setup: All data were acquired on a 3T Prisma system (Siemens
Healthcare, Erlangen, Germany) using a body coil array. The study protocol included
a free-breathing radial stack-of-stars 3D GRE (RAVE) sequence with golden-angle
acquisition. It was tested on 15 healthy human volunteers. RAVE imaging parameters included oversampling
factor=2, TR/TE=4.0/1.7ms, BW=500Hz/pixel, 240 slices, 800 radial views, 1.6mm isotropic
resolution.
Principle: A
prototype PT transmitter is a small device placed outside the MR bore with no
direct contact with the patient. Physiological movement of the subject causes
coil load variations, resulting in modulations of the PT signal detected by the
MR receive coil. The PT signal frequency is controlled so that it is imprinted
outside the object in image space. To avoid interference between the PT signal and
the MR signal (center frequency at 3T = 123.25 MHz), the PT is tuned to
transmit ~100 kHz off-resonance. The separation between the imaged object and the
pilot-tone (Fig. 1a) is noticeable after FT along the frequency domain. The image
(Fig. 1b) and PT (Fig. 1c) information can be separated and a respiratory
signal can be extracted by a fit in the frequency domain:$$A\cdot\exp\left(-i\cdot2\pi\cdot\ f\cdot\ t\right)$$ where $$$ f$$$ is the PT frequency and $$$ A$$$ is the complex amplitude signal, which modulates in accordance with the respiration (Fig. 1d). A peak-detection
algorithm calculates the PT’s frequency based on the strongest coil and then
uses this frequency to calculate the coefficient ($$$A$$$) and its modulation over time for the rest of the coils.
Workflow: During experiments, the PT transmitter is placed outside the MR bore, resulting in a unique signal imprinted in the image data prior to processing (Fig.
2a). The breathing-related PT signal modulation,
picked up by each receive coil, is extracted by the peak-detection algorithm and
processed by principal component (PCA) analysis, resulting in one respiratory
signal from all coils (Fig. 2b). As the next step, the respiratory signal is
exploited by an eXtra-Dimensional (XD) reconstruction pipeline (3), which bins the continuously acquired radial data into different
respiratory states from inhale to exhale (Fig. 2c).RESULTS AND DISCUSSION
When comparing respiratory signals from
the respiratory belt (Fig. 3a, blue), self-navigation (Fig. 3a, red), and pilot
tone (Fig. 3a, green), similar patterns were seen for self-navigation and PT,
but the belt signal differed from those patterns. The belt is an analog device
that is sensitive to the patient setup, often leading to distorted/clipped
signal as experienced here. Similarity between the PT and k-space center
signals was noted whether the subject was breathing steadily (Fig. 3b) or
unsteadily (Fig. 3c). To reduce dimensionality and noise, PCA analysis, second-order
blind identification (SOBI) (5), and coil clustering (6) algorithms were used (Fig.
4a) to process the signals recorded by all MR coils. Respiratory signals based
on k-space center (Fig. 4a, pink) missed some respiratory information while PT
showed better signal recurrence when processed by the different methods. This
result has a direct impact on how motion affects the final images (Fig. 4b),
revealing clearer anatomical details like the pancreas and the abdominal wall
when using the PT. Moreover, it also influences the image quality along the
different respiratory motion states. In a 3D view of another volunteer, use of
the PT signal resulted in less motion blurring especially at the liver tip and in
the center of liver (Fig. 4c). To further illustrate the reliability of PT, a video
of zero-angle acquisitions after Fourier
transformation shows how the PT signal (blue) is synchronized with the
actual breathing of the subject (Fig. 5).CONCLUSION
A novel device for tracking respiratory motion,
called a pilot tone, showed fewer motion artifacts when compared to conventional
k-space self-navigation and respiratory belts. The small dimensions (8 cm) and high sampling rate associated with the PT, offer great potential for tracking
breathing signals. Additionally, since the pilot-tone retrieves its
information separately from the MR data, it is well suited to tracking motion during
the injection of contrast material, which is not possible with k-space-based
signals due to spatially varying contrast uptake.Acknowledgements
We acknowledge support from NIH grant P41
EB0171813 and R01 5R01EB018308.References
- Havsteen
I, Ohlhues A, Madsen KH, Nybing JD, Christensen H, Christensen A. Are Movement
Artifacts in Magnetic Resonance Imaging a Real Problem?-A Narrative Review.
Front Neurol 2017;8:232.
-
Zaitsev M, Maclaren
J, Herbst M. Motion artifacts in MRI: A complex problem with many partial
solutions. J Magn Reson Imaging 2015;42(4):887-901.
-
Feng
L, Axel L, Chandarana H, Block KT, Sodickson DK, Otazo R. XD-GRASP:
Golden-angle radial MRI with reconstruction of extra motion-state dimensions
using compressed sensing. Magn Reson Med. 2016 Feb;75(2):775-88.
-
Speier P, Fenchel M, Rehner R, PT-Nav: a
novel respiratory navigation method for continuous acquisitions based on
modulation of a pilot tone in the MR-receiverProc. ESMRMB 2015, 128: 97-98.
- Belouchrani A,
AbedMeraim K, Cardoso JF, Moulines E. A blind source separation technique using
second-order statistics. Ieee T Signal Proces 1997;45(2):434-444.
-
Zhang T, Cheng
JY, Chen YX, Nishimura DG, Pauly JM, Vasanawala SS. Robust Self-Navigated Body
MRI Using Dense Coil Arrays. Magnetic Resonance in Medicine 2016;76(1):197-205.