Synopsis
Magnetization transfer (MT) imaging is
sensitive to changes in the macromolecular content of tissue and is, therefore,
gaining increased attention as a noninvasive approach to
probe the complex tumor environment in cancer. The ratio of macromolecular
protons to the protons in the free water pool, or pool size ratio (PSR), can be
quantified with quantitative MT (qMT) imaging and may be useful for detection
of changes in macromolecular content early in the course of treatment. In this
study, we explore the repeatability of PSR measurements in healthy breast
fibroglandular tissue at 3T to serve as a benchmark for future longitudinal
studies of breast cancer treatment.Introduction
Magnetization
transfer (MT) imaging is sensitive to changes in the macromolecular content of
tissue and is, therefore, gaining increased attention as a noninvasive approach
to probe the complex tumor environment in cancer
1,2. We previously demonstrated the reproducibility
of magnetization transfer ratio (MTR) measurements in fibroglandular tissue of
the breast
3; however, MTR is a semi-quantitative measurement
dependent upon several factors, including the pulse sequence parameters and
tissue relaxation characteristics.
Quantitative MT (qMT) imaging is a technique that potentially provides more
specific information on tissue composition,
including the ratio of macromolecular protons to the protons in the free water pool,
or pool size ratio (PSR)
4. The aim of this
study is to explore the reproducibility of PSR measurements of fibroglandular
(FG) tissue in healthy controls at 3T.
Methods
Six
women (mean age: 40 years, range: 27-54 years) with no history of breast disease
were scanned twice during a single visit: the protocol was run once, the
volunteers were taken off the table to stretch then repositioned, and the
protocol was repeated. Images were acquired with a 3T Achieva MR scanner
equipped with the MammoTrak table, including a dedicated 16-channel sensitivity
encoding (SENSE) receive double-breast coil (Philips Healthcare, Best, The
Netherlands). For qMT imaging, a MT-prepared (20 ms sinc-Gauss
pulse), segmented EPI sequence (5 lines/shot) with a water-selective excitation
pulse (1331, 6°), flow-compensation, and respiratory gating was employed. Data
were collected at four MT offset frequencies (1, 2, 4 and 8 kHz) using two MT
pulse angles (500° and 800°, plus one image at 0° for normalization), resulting
in 9 volumes in a nominal scan time of 1 min 38 s. Additional parameters
included: acquired (reconstructed) resolution = 2×2×5 mm
3
(1.33×1.33×5 mm
3),
TR/TE = 48/6.6 ms, and SENSE factor = 1.5. The qMT model requires independent
T1,
RF transmit (
B1+),
and main magnetic field (∆
B0)
estimates.
T1
was estimated using the multiple flip angle
(MFA) method with 10 flip angles (2:2:20°) and TR/TE = 7.9/4.6 ms.
B1+
was measured using a Bloch-Siegert method
5.
∆
B0
was measured using a dual-gradient echo method with fat and
water protons in phase. All
data were non-rigidly co-registered to the reference qMT volume (Advanced
Normalization Tools) and fit to a two-pool model to estimate PSR and the
T2 of the macromolecular
protons. During fitting, the
T1/
T2 of water protons (40), and
the MT rate (48 Hz) were fixed to published values in skeletal muscle
6.
The
reproducibility of the median PSR (mPSR) for fibroglandular (FG) tissue was determined by evaluating the 95% CI of the mean
difference, within-subject standard deviation (wSD), and repeatability
coefficient (r) with the test-retest
sessions
7.
Results
Median fibroglandular PSR values for
each volunteer are listed in the
Table.
PSR maps from the central slice of each subject for scan 1 (top row) and scan 2
(bottom row) are shown in
Figure 1.
FG PSR values are plotted for each data set, with the median values denoted by
the solid lines (
Figure 2a). The
difference between the mPSR values between scans is plotted against the average
of the mPSR values for the two scans (
Figure
2b). The mean difference for all subjects (0.15) was not significantly
different from zero, and the individual difference values were not dependent
upon the average mPSR value. The 95% confidence interval limits were ±1.07 (α =
0.05) and the repeatability measure (2.77 × wSD) was 2.07.
Discussion
qMT
imaging is potentially sensitive to changes in glycoprotein content in the
extracellular matrix, which is known to change during the tumor life cycle and
in response to treatment8; thus, it is a reasonable hypothesis that
qMT parameters may change during the course of therapy and potentially be
useful for predicting treatment response. However, prior
to applying qMT imaging to assess treatment response, it is necessary to have an
expectation of the typical variation in the PSR of healthy breast tissue. To the authors’ knowledge, this is
the first application of qMT in the breast, resulting in reasonable reproducibility
of PSR measurements with a clinically feasible sequence.
It is
noted that the accuracy of the model fit may be reduced because of several
factors, including a reduced number of offsets to keep the qMT sequence as
short as possible, the fixed values used in the fitting process, partial volume averaging of adipose and fibroglandular
tissue in the relatively large voxels, and volunteer motion between the B1+, B0, T1, and qMT acquisitions. Future work includes addressing
these issues and applying this technique in an ongoing multi-parametric study to
predict treatment response9.
Acknowledgements
R25CA092043, U01CA142565, U01CA174706References
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