Toshimasa James Clark1, Gregory J Wilson2, and Jeffrey H Maki2
1Department of Radiology, University of Colorado Denver, Aurora, CO, United States, 2Department of Radiology, University of Washington, Seattle, WA, United States
Synopsis
CE-MRA spatial resolution is determined by a complex
interaction between acquired voxel size, gadolinium injection rate, contrast volume,
cardiac output, magnetic field strength, and acquisition duration. R1 relaxivity
non-linearity and R2* signal degradation inherent in SPGR acquisitions play
important roles in observed signal intensity during bolus passage. Through
generation of modulation transfer functions spanning the gamut of parameter
values likely to be seen in clinical practice we derive injection rates that
produce optimal image contrast and resolution in our model.Purpose
Optimization of high resolution contrast-enhanced magnetic
resonance angiography (CE-MRA) is a non-trivial problem due to the linked
interactions of acquired voxel size, sequence duration, bolus timing, contrast
recirculation, and desirability to maintain R1 enhancement throughout the
acquisition of k-space without inducing R2*-related reduction of signal. Some investigators
indicate superior resolution and image contrast may be achievable with slower
gadolinium injection rates than those typically applied. We seek to further evaluate this hypothesis.
Methods
We applied a computer-based model implemented in MATLAB
(Mathworks, Natick, MA) to measure both resolution and image contrast through
analysis of generated modulation transfer functions (MTF). [1] Contrast
injection volume and rate, cardiac output, magnetic field strength, and elliptical-centric
image acquisition parameters were varied over a wide gamut. We modeled the
effects of gadobenate dimeglumine, although the model allows for simulation of
other gadolinium formulations. Recirculation was modeled, with parameters
chosen to approximate levels observed in healthy volunteers (unpublished data),
with baseline signal-to-noise ratio (SNR) ranges derived from clinical renal
and carotid examinations. Ultimately, a
MTF was generated for each discrete set of parameters. Resolution at which 50%
absolute modulation transfer is achieved (MTF50%), maximum SNR achieved at the optimal
(i.e., minimum MTF50%) injection rate
(SNRmax), and area under the modulation transfer curve (AUC) were recorded for
each run, with parameter combinations resulting in maximum SNRs of less than 10
excluded from analysis as non-diagnostic. [2]
Each set of 0.1-5.0 mL/sec injection rate data acquired at a
particular combination of parameters was analyzed, with the injection rates
resulting in minimal resolution loss (minimum MTF50%) and maximal image
contrast (maximum AUC) recorded. Modulation transfer curves were exported
directly, AUC and MTF50% data were visualized as a scatter plot, and 3-D
surface renderings were created from these data.
Results
Modulation transfer functions vary significantly with
injection rate and imaging parameters (Figure 1). Generally, the height of the initial
plateau (left side of graph) represents the maximum contrast concentration
during the bolus, and varies surprisingly little with injection rate. The subsequent downslope and nadir (right side
of graph) represent recirculatory effects.
Acquisition at 1.5T (vs. 3.0T)
does not significantly alter optimal injection rates (not depicted), although it
does result in lower observed SNRs. Maximum area under the MTF curve typically
occurs at slightly higher injection rates than does minimum MTF50% (Figures 2,
3, and 4). Optimal resolution for typical breath-hold renal CE-MRA is achieved
with injection rates on the order of 0.5-1.0 mL/s, dependent on contrast
injection volume, whereas for carotid these rates are on the order of 0.2-0.3
mL/s (Figure 3). Maximum SNR varies with both contrast injection volume and
cardiac output, with slightly greater variance across the gamut for carotid
imaging parameters (Figure 5).
Discussion
Optimization of spatial resolution and vessel contrast in
CE-MRA is non-trivial. In particular, increasing gadolinium concentration does
not always lead to increased signal intensity. Recent work indicates that the
whole blood gadolinium concentration must remain at a level that produces high
R1 relaxation without inducing R2*-related reduction of signal. [3, 4]
Most prior investigation of the relationship between
gadolinium injection rate in CE-MRA and resulting resolution and image contrast
has been hindered by use of subjective measures of image quality. Multiple
extant studies in which the authors attempted to define imaging parameters to
optimize CE-MRA image quality also have the limitation of no systematic
variation in injection rate, or the choice of several discrete injection rates.
Using a computer-based model allowed us to explore a wide
gamut of injection rates, contrast volumes, and cardiac outputs, and we created
objective metrics based on the modulation transfer function. We found that
cardiac output, contrast injection volume, and image acquisition times all
affect the optimum injection rate for which maximum area under the MTF curve
and resolution is achieved.
This
work suggests optimal image resolution is achieved at intuitively slow
injection rates (0.2-1.0 mL/s, dependent on imaging parameters). Higher
injection rates rely purely on recirculation to maintain R1 enhancement during peripheral
k-space acquisition, and this modeling suggests that this leads to significant
resolution loss.
This work suggests that slower injections better optimize resolution
by virtue of the longer injection duration, allowing for greater uniformity of R1
enhancement throughout k-space acquisition. This increased resolution comes
with only a minimal loss of SNR due in part to the non-linearity of R1
relaxivity and the R2* degradation seen with high gadolinium concentrations, as
can be seen graphically in our modulation transfer function curves (Figure 1).
Acknowledgements
No acknowledgement found.References
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Resolution Limitations in Contrast-Enhanced MRA Related to the Contrast Bolus
Profile using an Analysis of the Modulation Transfer Function. Presented at the
ISMRM 2014 Joint Annual Meeting; Milan, Italy.
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accuracy and precision as a function of MR imaging parameters and boundary
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resonance in medicine: official journal of the Society of Magnetic Resonance in
Medicine / Society of Magnetic Resonance in Medicine 2013.
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International Society of Magnetic Resonance in Imaging 21st Annual Meeting &
Exhibition; 2013; Salt Lake City, UT.