Christiana Sabett1, Ariel Hafftka1, Kyle Sexton2, and Richard Spencer2
1Applied Mathematics & Statistics, and Scientific Computation (AMSC), University of Maryland, College Park, College Park, MD, United States, 2National Institute on Aging (NIA), Baltimore, MD, United States
Synopsis
Magnetic resonance (MR) relaxometry time distributions are
recovered via the inverse Laplace transform (ILT), an ill-posed problem that is
generally stabilized using Tikhonov regularization. Recent work has considered
other penalties, such as the L1 penalty for locally narrow distributions. Lp
penalties, 1<p<2, may be appropriate for distributions consisting of both
narrow and broad components; a linear combination of L1 and L2
penalties, the elastic net (EN), may similarly be useful. However, there is
little guidance regarding the choice of regularization penalty for the recovery
of transverse relaxation distributions. We compare the effectiveness of each
penalty for representative relaxation data.
PURPOSE
Magnetic resonance (MR) relaxometry is an emerging technique for characterizing
biological tissues.1-3 Relaxation
time distributions are recovered via the inverse Laplace transform (ILT), an
ill-posed problem. This procedure is most often stabilized using Tikhonov
regularization with an L2 penalty, defined as the sum of the squared
elements of the solution vector. Recent advances in computational methods and
interest in sparsity have motivated additional work evaluating other
penalties. The promotion of sparsity by
the L1 penalty is suitable for locally narrow transverse relaxation
distributions.4 Lp penalties,
1<p<2, may be appropriate for distributions consisting of a combination
of narrow and broad components; similarly, a linear combination of L1
and L2 penalties, the elastic net (EN), may be useful in such
circumstances. However, there is little specific
guidance regarding the choice of regularization penalty for the recovery of MR
relaxation data. Here, we compare the effectiveness of each penalty for representative
relaxation data.THEORY
The discrete
measured signal takes the form
y(ti)=K∑j=1F(T2,j)e−ti/T2,j
where y(ti) denotes
signal amplitude at acquisition times ti, typically integral multiples of an echo time
(TE), T2,j denotes the decay
time constant of the jth component,
and F(T2,j) is its associated
magnitude. In matrix form:
y=AF
where
[A]i,j=e−ti/T2,j,1≤j≤K
is the n×K kernal, y is the length-n vector representing measurements at time points ti,1≤i≤n, and F is a length-K vector of amplitudes corresponding to possible relaxation times. With Tikhonov
regularization, recovery of F is cast as a nonnegatively
constrained regularized least squares problem,
minF≥0{||AF−y||22+α2||F||22}
where α weights the regularization
term relative to the fit residual. Similarly, for the L1 penalty, we
have
minF≥0{||AF−y||22+α||F||1}
while the Lp
penalty appears as
minF≥0{||AF−y||22+α||F||p}
and the EN
penalty as
minF≥0{||AF−y||22+α1||F||1+α2||F||2}
METHODS
Our input model consists of a
bimodal T2 distribution with Gaussian peaks, each characterized by
mean T2 and standard deviation (SD). For Lp penalties,
the regularization parameter was established within a range of [10-7,10-1]. For the EN penalty, a 5×5 grid search was performed across a
range of [10-6,10-2] for α1 and a range of
[10-7,10-3] for α2. Minimizations
were performed using CVX software.5 The unknown model vector F consisted of 176 allowable T2 rates, logarithmically spaced between 10 and 1000 ms. Noise-free decay data was generated at 352
discrete TE values, and then corrupted with additive white Gaussian noise,
appropriate for spectroscopic or high signal-to-noise imaging experiments. Performance
was evaluated using mean-squared error between the input model and the
recovered distribution, normalized by the sum of the squared values of the
input model. RESULTS
Figure 1
demonstrates the superiority of the L1 penalty in recovering a
narrow distribution (Fig. 1a), and the superiority of the L2 penalty
in recovering a wider-peak distribution (Fig. 1b). The heat maps in Figure 2a and 2b show performance
across a range of models with varying (but equal in each peak) linewidths, and varying separations,
for the L2 and L1 penalties, respectively. The L2 penalty is seen to perform well
overall, but poorly for overlapping peaks.
The L1 penalty clearly begins to fail as peak width increases, as
expected. Figure 3 defines the optimal
penalty across the same range of linewidths and peak separations. For a
distribution of peaks of unequal SD, Figure 4 shows better performance by the L1.5
penalty as compared to the L2 penalty. Finally, Figure 5
demonstrates T2 distribution recovery for normal and osteoarthritic
human cartilage samples,1 showing that all penalties recovered a bimodal distribution with roughly
consistent peak centers but with markedly different peak SD. Based on our simulation analysis, we expect
that the L1.5 recovery is likely to be the most appropriate.DISCUSSION
For sparse distributions, we
find that the L1 penalty
is optimal. The L2 penalty performs very well across a wide range of
parameter values, underscoring the robustness of conventional Tikhonov
regularization. Of particular interest
are distributions with unequal peak widths, where neither the emphasis on
sparsity from the L1 penalty nor the emphasis on smoothness in the L2
penalty are fully optimal. We found that the L1.5 and EN penalties were more successful in modeling this situation. Of
these the elastic net promotes sparsity, but requires optimization over two
regularization parameters, so that the L1.5 may be preferred overall.
Overall, our results demonstrate the regions where the use of a particular regularization
penalty term is likely to be most appropriate, and can be implemented in the
usual case in which the experimentalist has a priori knowledge of the general characteristics of an underlying
model distribution.Acknowledgements
This work was supported by
the Intramural Research Program of the NIH, National Institute on Aging. We thank John Benedetto and Alfredo Nava-Tudela
of the University of Maryland for their interest and comments. Tissue samples were kindly provided by Dr.
Tariq A. Nayfeh.References
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