Alexander Joos1, Olga Mykhaylyk2, Norbert Löwa3, Dietmar Eberbeck3, Bernhard Gleich1, and Axel Haase1
1Zentralinstitut für Medizintechnik der Technischen Universität München, Garching, Germany, 2Department of Experimental Oncology, Klinikum rechts der Isar der TU München, Munich, Germany, 3Physikalisch-Technische Bundesanstalt, Berlin, Germany
Synopsis
Magnetic
nanoparticles can be used for magnetic drug targeting while MRI can
serve as non-invasive therapy monitoring. We investigated the
influence of the assembling of magnetic nanoparticles with oncolytic
viruses and their uptake into cancer cells on the MRI relaxivities
r1, r2 and r2* and magnetically characterized all samples using
magnetic particle spectroscopy. Our results show that R2*
measurements seem most suitable for particle quantification while R2
is sensitive to the uptake of the particles into the cells. Magnetic
particle spectroscopy proves to be an important validation technique
for MRI relaxometry.Introduction
Magnetic
nanoparticles (MNPs) can be used as carriers for magnetic drug
targeting 1. When assembled with oncolytic viruses they
are a promising tool for cancer treatment. The contrast enhancing
properties of these particles in MRI allow for non-invasive therapy
monitoring. Our goal is to investigate how MRI relaxometry can be
used to assess the spatial distribution of the particle concentration
and the aggregation state of the MNP-virus-complexes in the tissue of
interest.
For
this purpose, we studied the influence of the assembling of MNPs with
oncolytic viruses and their uptake into cancer cells on the MRI
relaxivities r1, r2 and r2*.
In
addition, all samples were magnetically characterized using magnetic
particle spectroscopy (MPS). MPS has been proven a
straightforward technique for quantification and characterization of
MNPs and allows for the validation of MRI relaxation
measurement results.
Methods
PEI-Mag2
(PM) and SO‐Mag5 (SO)
magnetic nanoparticles were assembled with oncolytic adenovirus (Ad)
as described previously 2. Multi drug resistant human
pancreatic carcinoma (RDB) cells were labelled with PM and SO
nanoparticles and infected with magnetic Ad complexes.
Both
particles were also assembled with oncolytic vesicular stomatitis
virus (VSV). Rat Morris hepatocellular carcinoma
(McA) cells were labelled with PM and SO nanoparticles
and infected with magnetic VSV complexes.
Dilution
series of all sample types were prepared and embedded in agarose. R1,
R2 and R2* relaxation
rates were measured on a 3 T whole body imaging system (GE
Discovery MR750w) using spin echo inversion recovery, (single) spin
echo and multi-echo gradient echo sequences. ROI signal intensities
were least-squares fitted for each voxel with three-parameter fits.
A commercial magnetic particle spectrometer (Bruker
BioSpin) was used to measure the spectral response to an oscillating
magnetic field (Bexcit=25
mT, f0=25
kHz, T=37°C)
of the samples.
Results and Discussion
For
clarity, only exemplary data is shown here. Figures 1-3 show the
relaxation rates of the dilution series of PEI-Mag2 nanoparticles
homogeneously suspended in agarose, assembled with adenovirus, after
internalization in RDB cells and assemblies with adenovirus after
internalization in RDB cells. Relaxivities are summarized in Table 1. r1
and r2 relaxivities do not change significantly
when the complexes are formed but drop when the particles are
absorbed by the cells. Within the error margins, r2*
relaxivites are very similar in all samples.
The
MPS results of the dilution series demonstrate a highly linear
correlation between the signal amplitude A3 and the
iron amount mFe for PEI-Mag2 and SO-Mag5 samples.
The shape of the MPS spectra, expressed as the A5/A3
ratio, was not affected by dilution within uncertainty limits for
samples with more than 0.5 μg iron. As the A5/A3
ratio
is a strong indicator for a changing magnetic response, the results
shown in Figure 4 indicate that the structure of the aggregates (and
therefore the magnetic interaction between the particles in the
aggregates) is largely the same for all samples. This can explain the
constant r1 and r2 relaxivities
for the free particles and the magnetic viral complexes. The
distribution of the aggregates in the sample (homogeneous in agarose
but more localized in the cells) has obviously no influence on the
magnetic interaction between the particles and therefore on their MPS
spectra, but does have an influence on the local interaction between
the particles and the water protons. This can explain the drop in r2
for particles/complexes internalized by the cells (partial refocusing
3).
However, lower concentrated samples show higher
deviations in their MPS spectra including some trends, which is not
reflected in the relaxation rates. Possible reason might be a changed
aggregate structure due to dilution accompanied by an altered
dipole-dipole interaction between MNPs within the MNP virus complex.
Conclusion
Since
r2* relaxivites are
very similar in all samples, R2* measurements seem most suitable for
particle quantification after a calibration step. r2
relaxivities, however, change significantly when the particles or the
magnetic viral complexes are internalized by the cells. Measurements
of R2 in addition to R2* could thus be used to detect whether the
particles are inside or outside of the cells. r1
relaxivities are very low for all samples, which is why they are
expected to give too little contrast in tissue for a quantitative
interpretation.
Our
results also show that additional MPS measurements are important for
the accurate interpretation of MRI relaxometry results because MPS
detects MNPs and their interaction directly whereas MRI can only
observe the interaction between particles and water protons.
Acknowledgements
No acknowledgement found.References
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