Vasily L. Yarnykh1
1Radiology, University of Washington, Seattle, WA, United States
Synopsis
Correction of B1 field
non-uniformity is critical for quantitative MRI methods including fast
macromolecular proton fraction (MPF) and variable flip angle T1 mapping. However,
B1 mapping sequences increase the examination time and are not
commonly available in clinics. A new algorithm is presented to enable
simultaneous B1 correction in R1=1/T1 and MPF mapping without acquisition of B1
maps. The principle of the algorithm is based on different mathematical
dependences of B1-related errors in R1 and MPF allowing extraction of a surrogate
B1 map from uncorrected R1 and MPF maps. The method demonstrated excellent
agreement with actual B1 mapping at 3T.
Introduction
Single-point
macromolecular proton fraction (MPF) mapping1,2 is a quantitative
MRI method for the assessment of myelination in neural tissues. MPF
demonstrated strong correlations with histologically measured myelin density in
animal models3-5 and showed a promise as a biomarker of myelin in
multiple sclerosis6,7 and brain development8-10 studies. In
the single-point synthetic-reference method2, MPF maps are reconstructed
from three source spoiled gradient-echo (GRE) images providing magnetization
transfer (MT), T1, and proton-density (PD) contrast weightings. One
limitation of this method is its sensitivity to errors caused by B1
field inhomogeneity rendering the need in B1 mappings as a part of
imaging protocols.11 However, B1 mapping sequences
increase the examination time and are not commonly available in clinical
settings. As an intermediate result, the single-point MPF mapping method1,2
produces R1=1/T1 maps reconstructed using the two-point
variable flip angle (VFA) method, which also require B1 correction.Purpose
To develop a
data-driven algorithm for simultaneous correction of B1 inhomogeneity
in MPF and R1 maps without actual B1 mapping.Theory
The idea of the proposed algorithm is to
exploit the distinctions in the mathematical description of B1-related
errors in MPF and R1 in order to reconstruct a surrogate B1
field map directly from uncorrected MPF and R1 maps and recursively
apply it for correction of initial MPF and R1 maps. A simplified
equation describing the MT-weighted spoiled GRE signal in the presence of B1
non-uniformity (expressed as the B1 scaling factor c=B1actual/B1nominal) was derived using
the first-order approximation of the matrix pulsed steady-stated MT model1
(Fig. 1, Summary of equations, Eq. [1]). Dependence of B1-related
errors in R1 and PD on c
was described earlier (Fig. 1, Eqs. [2] and [3]).12 Computation of
MPF with unknown B1
non-uniformity can be expressed as the fit of the signal model calculated with the nominal values of RF-related variables (c=1) and the measured values of PD and R1 containing B1-related errors (PDm
and R1m) to the
experimental signal given by Eq. [1] (Fig.
1, Eq. [4]). After solving Eq. [4] with Maclaurin series expansion for a small
flip angle (FA) α, an equation describing the relationship between measured and
actual MPF (fm and f) was obtained (Fig. 1, Eq. [5]). We
further assume a global linear relationship between R1 and MPF in the absence of B1 errors (Fig. 1, Eq. [6]), which implies that R1
variations in tissues are primarily determined by the macromolecular content,
while the variability due to paramagnetic ions is of the second order. After substituting
R1 and f from Eqs. [2] and [5] into Eq. [6],
the biquadratic equation for c can be
obtained with the solution given by Eq. [7] (Fig. 1). According to Eq. [7], a
surrogate B1 map can be reconstructed from uncorrected R1
and MPF maps with the knowledge of population-averaged constants r0 and rf, while other variables are the known constraints of the
single-point algorithm (R and T2B)1 and
sequence parameters.Methods
Participants: Data were obtained from 8 healthy volunteers (mean
age 44.6±12.2 years).
MRI Protocol: MRI
acquisition was performed on a 3.0 Tesla Philips Achieva scanner using a
previously described2 protocol including 3D PD- (TR=21 ms, FA=4°), T1-
(TR=21 ms, FA=25°), and MT-weighted (TR=28 ms, FA=10°, saturation offset
frequency 4 kHz, effective FA=560°) spoiled GRE sequences with isotropic
resolution of 1.25x1.25x1.25 mm3. AFI13 B1 maps (TR1/TR2=40/160
ms, FA=60°) were obtained with the voxel size of 2.5x2.75x5.0 mm3.
Image processing and
analysis: MPF and R1 maps were reconstructed using the single-point synthetic-reference
algorithm2 with three B1 correction options: no correction,
AFI, and the described data-driven algorithm. AFI-corrected MPF maps were automatically segmented into white matter (WM) and gray matter (GM) using FSL
software. The resulting tissue masks were applied to all maps to calculate mean
MPF and R1. The constants r0 and rf
were estimated from whole-brain voxel-based linear regression of R1
on MPF and averaged across subjects.
Statistical analysis: Repeated-measures ANOVA with post-hoc Tukey tests and Bland-Altman
plots were used to assess agreement between B1 corrections for MPF and R1 in WM and GM.Results
According to
simulations (Fig. 2), the absence of B1 correction results in large R1
errors (about four-fold overestimation at c=0.5)
and smaller but substantial MPF errors (~20-25% overestimation at c=0.5). These errors are almost completely eliminated
by the described algorithm (Fig. 2). Mean ± SD experimental
values of the algorithm constants were: r0=0.32±0.01 s-1 and
rf=4.73±0.10 s-1.
Surrogate B1 maps closely reproduced actual B1
field distribution (Fig. 3). R1 and MPF maps reconstructed without B1
correction showed significant bias in WM and GM measurements (P<0.001, Fig. 4) and apparent
propagation of spatially dependent B1-related errors (Fig. 3). Correction
of R1 and MPF maps using surrogate B1 field reduced the
bias to a non-significant level (P=0.77
and 0.12 for WM and GM R1 and P=0.10
and 0.10 for WM and GM MPF, Fig. 4) and markedly improved uniformity of the resulting
maps (Fig. 3). Conclusions
The data-driven algorithm
eliminates the need in B1 maps in the fast MPF and VFA R1
brain mapping techniques. If R1 (or T1) is of primary interest,
an additional MT-weighted scan can replace specialized B1 mapping
sequences in imaging protocols to enable B1 field correction.Acknowledgements
Grant support: NIH R24NS104098;
R21NS109727; R01EB027087.References
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