Hansol Lee1, Sun-Yong Baek2, Se Young Chun3, Jae-Hyeok Lee4, and HyungJoon Cho1
1Department of Biomedical Engineering, Ulsan National Institute of Science and Technology, Ulsan, Republic of Korea, 2Department of Anatomy, Pusan National University School of Medicine, Yangsan, Republic of Korea, 3Department of Electrical and Computer Engineering, Ulsan National Institute of Science and Technology, Ulsan, Republic of Korea, 4Department of Neurology, Pusan National University Yangsan Hospital, Yangsan, Republic of Korea
Synopsis
The overall goal of this work was to provide a truth of
neuromelanin-sensitive T1 weighted image with magnetization transfer effects
and to segment the respective distribution of neuromelanin-iron complex and
ferric iron within substantia nigra which are important to monitor Parkinson’s
disease. Postmortem MR experiment at 7T and histological validation were
performed for six normal midbrain samples. The correlation between T2*/T2 and
neuromelanin pigments was highest compared to other MR parameters, especially
compared to T2*, which shows specific distributions of paramagnetic molecules.
Iron deposits were highly correlated with iron-sensitive T2 and T2* and the
correlation was reduced for T2*/T2.
Purpose
Neuromelanin (NM) is a dark
pigment which chelates iron in dopaminergic neurons of human substantia nigra
(SN).1 Parkinson's disease (PD) is a major
progressive nervous system disorder associated with the increase of ferric
iron deposition and the loss of dopaminergic neurons.2 To define the distribution of paramagnetic molecules such
as NM-iron complex and ferric iron in SN is meaningful to examine PD
progression. Several studies have reported T1 weighted image with magnetization
transfer (MT) effects provides NM-sensitive MR contrast.3 However, both
NM-iron complex and ferric iron are paramagnetic molecules due to the load of highly
concentrated iron on NM for preventing oxidative stress to the tissue.4
They cause the variation of magnetic field and affect T2 and T2* values.5
T2 and T2* values were also influenced by both concentration and practical
size difference of the magnetic sources.5 The aim of this study was
to specifically clarify the respective visualization of NM-iron complex and ferric iron within
SN by combining MR relaxation times, T2 and T2*.Methods
The midbrain pieces including
SN were extracted from elderly individuals without any diagnosis of neurodegenerative
diseases. The study design for postmortem experiments was approved by the
appropriate ethics review boards. The postmortem MR experiments were conducted at the
preclinical 7T MRI system (Bruker, Germany). The formalin fixed samples were
scanned for the T1 weighted image with and without MT effects, T1 map, T2 map,
T2* map, QSM, and SWI. T1 weighted image with MT effects was acquired by multi
slice RARE sequence with and without MT pulses, which are two sequential sinc
pulses of 1 kHz off-resonance and 600 ĚŠ flip angle. T1, T2, and T2* maps were
reconstructed using non-linear least-square fit on the RAREVTR, MSME, and MGE
signals. T2*/T2 values were acquired voxel by voxel. QSM and SWI were generated
using both magnitude and phase data of the MGE signal. After ex vivo MR
experiments, the midbrain pieces were cryoprotected in sucrose solution. The
samples were sectioned to 50 μm-thick slices according to the corresponding T1
weighted images. The slices were stained with Perls' Prussian blue staining for
ferric iron and Luxol fast blue (LFB) staining for myelin. Binary images of NM
and iron were detected from Perls’ Prussian blue staining. The binary image of
myelin was detected by LFB staining. The Pearson’s correlation coefficients
were calculated from iron density and NM density with MR parameters.Results
The hypointense region in T1
weighted image with MT effects was closely linked to the myelin distribution of
LFB staining which was validated in Figure 1. NM-iron complex and ferric iron,
which are paramagnetic molecules in SN detected from Perls’ Prussian blue
staining (Figure 2D), contributed to T2* shortening with their spatially
overlapped distributions. T2 map (Figure 2F) presented the distribution of ferric
iron without that of NM. The effect of iron on T2* map (Figure 2H) was
significantly reduced in T2*/T2 map (Figure 2I) only leaving the effect of
NM-iron complex. The paramagnetic property of NM by iron chelation and the
diamagnetic property of myelin were demonstrated by QSM (Figure 2C). The table
for Pearson’s correlation coefficients (Table 1) showed NM pigments were highly
correlated with T2* than T1 and T2. And iron deposits were sensitive to T2 and
T2* than T1. The T2*/T2 showed the highest correlation coefficient with NM
pigments than other MR parameters.Discussion
T1 weighted
imaging with MT effects was performed to delineate NM
distribution. T1 weighted image with MT effects and LFB staining showed that
the hypointense region was significantly matched with the myelinated region. The
hyperintense area in T1 weighted image with MT effects represented the
non-myelinated region. Because NM and myelin were not colocalized, the
hyperintense area in T1 weighted image may indirectly correlate with NM
distribution. As the MT effect has been used to measure myelin content, our results
were consistent with previous works.6
The distributions
of paramagnetic ferric iron and NM-iron complex were identified in usual T2*
map with overlapping when the T2* map was compared to the detected NM pigments
and iron deposits, respectively. Furthermore, the region of low T2*/T2 values was mostly
associated with NM distribution. The change of correlation coefficients
from T2* to T2*/T2 was higher for the density of NM pigments but lower for the
density of ferric iron deposits due to their effective size difference.
Therefore, the segmented region of NM-iron complex from T2*/T2 map and ferric
iron from T2 map can be obtained with the boundary of the SN decided from the
T1 weighted image.Acknowledgements
This
work was supported by the National Research Foundation of Korea under Grant No.
2017R1A1A1A05001062,
which is funded by the Korean Government. This
work was also supported by the 2017 Research
Fund (1.170017.01) of the Ulsan National Institute of Science and Technology
(UNIST).References
1. Zucca FA, Segura-Aguilar
J, Ferrari E, Muñoz P, Paris I, Sulzer D, Sarna T,
Casella L, and Zecca L, “Interactions
of iron, dopamine and neuromelanin pathways in brain aging and Parkinson's
disease”. Progress in neurobiology, 155, 96-119. (2017).
2. Damier
P, Hirsch EC, Agid Y, and Graybiel AM, “The substantia nigra of the human
brain”. Brain, 122(8), 1421-1436. (1999).
3. Sasaki
M, Shibata E, Kudo K, and Tohyama K, “Neuromelanin-sensitive MRI”. Clinical Neuroradiology, 18(3), 147-153. (2008).
4. Enochs
WS, Petherick P, Bogdanova A, Mohr U, and Weissleder R, “Paramagnetic metal
scavenging by melanin: MR imaging”. Radiology, 204(2), 417-423. (1997).
5. Hardy
PA, and Henkelman RM, “Transverse relaxation rate enhancement caused by
magnetic particulates”. Magnetic
resonance imaging, 7(3),
265-275. (1989).
6. Schmierer
K, Scaravilli F, Altmann DR, Barker GJ, and Miller DH, “Magnetization transfer
ratio and myelin in postmortem multiple sclerosis brain”. Annals of neurology, 56(3), 407-415. (2004).