Sungheon Gene Kim1,2, Eric Sigmund1,2, Melanie Moccaldi1,2, Thorsten Feiweier3, and Linda Moy1,2
1Center for Advanced Imaging Innovation and Research, Radiology, New York University School of Medicine, New York, NY, United States, 2Bernard and Irene Schwartz Center for Biomedical Imaging, Radiology, New York University School of Medicine, New York, NY, United States, 3Siemens Healthcare GmbH, Erlangen, Germany
Synopsis
This study is to investigate the
potential of the surface-to-volume ratio obtained from multiple diffusion times
to measure mammary duct microstructural changes induced by hormonal variation. Seven premenopausal women were scanned twice using a
stimulated-echo diffusion sequence; one in the follicular phase of the menstrual
cycle and again in the luteal phase. In 6 out of 7 subjects, the
surface-to-volume ratio measured with 69 and 173 ms was significantly reduced
in the luteal phase compared to the follicular phase. The length scales
obtained in our study are consistent with the duct diameters reported in
previous ex-vivo studies.PURPOSE
Recently, it has
been reported that the fractional anisotropy of fibroglandular tissue (FGT)
increases significantly when a longer diffusion time is used.
1 Furthermore,
it was reported that the ADC measurement with same
b-value and multiple diffusion times can be used to estimate the
surface-to-volume ratio (SVR) of the microstructural component that restricts
water diffusion, which was proposed to be dominated by mammary duct inner lining.
2
This study is to investigate the potential of the SVR measured from multiple
diffusion times as a novel marker for the microstructural changes of the
mammary duct induced by the hormonal variation during the menstrual cycle.
METHODS
Seven asymptomatic,
premenopausal women (32±7 years) were scanned twice; once in Week2 (follicular
phase) of the menstrual cycle and again in Week4 (luteal phase). All scans were
performed using a whole-body MAGNETOM Trio 3T scanner (Siemens Healthcare, Erlangen, Germany) with
a 7-element breast coil array. We measured diffusion using a prototype
stimulated-echo acquisition mode (STEAM)-DTI sequence with an echo-planar
imaging (EPI) readout and SPAIR fat suppression (TR/TE = 11500/45 ms, matrix =
192x132x10, resolution = 2.1x2.1x5 mm3, 6 directions, 3 averages,
parallel imaging factor = 2) with two different b-values (0 and 500 s/mm2).
The acquisition was repeated using 4 different diffusion times (Δ=69, 173, 466
and 903 ms) by varying the mixing time.
Diffusion-weighted
images were corrected for eddy-current-induced distortion using a non-affine
registration. The contribution of the imaging gradients was included in the
b-matrix for tensor estimation. Parametric maps of mean diffusivity (MD),
fractional anisotropy (FA), axial diffusivity (AD), and radial diffusivity (RD)
were derived from the diffusion eigenvalues (λ1, λ2 and λ3)
with AD = λ1 and RD = (λ2+λ3)/2. Regions of
interest (ROI) were manually drawn to select the FGT in the bilateral breast of
all imaging slices. For the voxels in the ROI, selection criteria of AD >
1.0 μm2/ms and AD < 2.7 μm2/ms were used to exclude any
voxels with a substantial partial-volume effect, with unsuppressed fat or
noise, respectively. The selected voxels were then used to quantify the
diffusion characteristics of the FGT using a bootstrapping analysis: the eigenvalues
were calculated from the average data of randomly selected 30% of the selected voxels
for each diffusion time; this process was repeated 500 times to calculate the
mean and standard deviation of the FGT diffusion metrics. With the RD values of
diffusion times 69 and 173 ms, surface-to-volume ratio (SVR) was calculated
using the Mitra short time limit model3: $$D(\Delta)=D_0[1-SVR\frac{4\sqrt{D_0\Delta}}{6\sqrt{\pi}}]$$
RESULTS
Figure 1 shows
representative images of one subject at two diffusion times, 69 and 173 ms,
that show reduced diffusivity at Δ=173ms,
compared to Δ=69ms.
This trend was consistently observed in all subjects. Figure 2 shows the
eigenvalues combined from all subjects in Week2 and Week4. At both menstrual
periods, the decrease of the RD was mostly between 69 and 173 ms. Figure 3 shows that the mean AD and RD measured with
69 and 173 ms did not change noticeably between Week2 and Week4. However, the
SVR was significantly reduced in Week4 for 6 out of 7 subjects as shown in
Figure 4, highlighting the potential benefit of individualized model fitting.
DISCUSSION and CONCLUSION
Assuming that
mammary ducts are the main underlying component in the fibroglandular voxels,
the SVR values can be converted to the diameters of a cylindrical model (d=4/SVR). Few studies have
explored the size of the milk ducts in the non-lactating breast. Taneri et al
4
reported a mean diameter of 0.57 mm in their series of 226 nipples, and Rusby
et al
5 reported a diameter of 0.7 mm at 3 mm beneath the nipple.
These diameters are about 2-3 times larger than what could be estimated from
our SVR values. Note that our measurement includes the entire ductal tree rather
than only the sub-areolar region. The discrepancy might also be due to the
difference between in-vivo and ex-vivo measurements. Nevertheless, the length
scales obtained in our study are in the same order of magnitude as in these
previous reports. Hence, the findings of this study suggest that the SVR
measurement may be used as a means to measure the average duct size of the FGT
in vivo. The ability to non-invasively
measure hormonal dependent changes in the size of lactiferous duct may allow
for improved characterization of these structural changes. A larger cohort of women is necessary to
determine if these normal fluctuations in the size of the milk ducts are also
seen in premenopausal women with breast cancer.
Acknowledgements
This work was supported by the NIH (CA160620).References
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