Alina Leandra Bendinger1, Christian Peter Karger2,3, Charlotte Debus4, Ralf Omar Floca3,5, Jürgen Debus3,6, Jörg Peter1, and Christin Glowa2,3,6
1Department of Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 2Department of Medical Physics in Radiation Oncology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 3Heidelberg Institute for Radiation Oncology (HIRO), National Center for Radiation Research in Oncology (NCRO), Heidelberg, Germany, 4Translational Radiation Oncology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 5Division of Medical Image Computing, German Cancer Research Center (DKFZ), Heidelberg, Germany, 6Department of Radiation Oncology, University Hospital Heidelberg, Heidelberg, Germany
Synopsis
Dynamic contrast-enhanced MRI was used for the longitudinal monitoring
of two well characterized experimental prostate tumors (Dunning R3327-AT1 and -HI)
after isodose and isoeffective radiotherapy. The effect of carbon (12C)-ion
irradition compared to photons on tumor vasculature was characterized by non-compartmental analysis and
pharmacokinetic modelling employing the extended Tofts model. Isodose and
isoeffective irradiation experiments indicated that the beam modality has a
stronger effect on tumor perfusion and permeability than the dose. While
changes in perfusion were identified for the highly undifferentiated AT1-tumor,
the more differentiated HI-tumor showed only minor changes in perfusion upon
irradiation.
Purpose
Carbon (12C)-ion radiotherapy (RT) provides enhanced biological
effectiveness relative to photon RT, especially for the treatment of
radioresistant tumors 1,2. In this longitudinal study, we employ dynamic contrast-enhanced MRI
(DCE-MRI) to compare treatment responses of two well characterized experimental
tumors after 12C-ion and photon RT.Methods
The anaplastic (AT1) and the more differentiated (HI) subline of the
Dunning prostate tumor R3327 3 were transplanted subcutaneously to both thighs of male Copenhagen rats
(AT1: 12 rats, HI: 16 rats). When tumors attained diameters of 10 mm, one tumor
per animal was irradiated with a single dose of either photons (6 MeV) or 12C-ions
(20 mm spread-out Bragg-peak), while the other served as untreated control.
AT1-tumors received 37 Gy photons or 12C-ions for isodose
experiments or 16 Gy 12C-ions or 85 Gy photons as isoeffective doses
to 37 Gy photons and 12C-ions, respectively. The HI-tumors were
irradiated with 37 Gy isodoses as well as with 18 Gy 12C-ions or 75
Gy photons (isoeffective treatments). DCE-MRI (TURBO-FLASH sequence, temporal
resolution: 0.75s, 380s total acquisition) was performed one day before and 3,
7, 14, and 21 days after irradiation (Fig. 1). Image signals were converted to
concentration by means of absolute signal enhancement. DCE-MRI data was
analyzed voxel-wise using an in-house developed software 4 by non-compartmental analysis (normalized area-under-the-curve, AUC), mean
residence time (MRT, defined as area under first moment curve) and by
pharmacokinetic modelling (PKM) using the extended Tofts model (ETM) 5. The image based arterial input function was extracted individually for
each animal from the left ventricle. Results were correlated with histology.
Results
3 days after irradiation, a clear increase in AUC-values was observed for
the AT1-tumors, while the control-tumors exhibited decreasing AUC-values (Fig.
2a). MRT elongated distinctly for control-AT1-tumors and slightly also for
photon-irradiated AT1-tumors (Fig. 2c). Low AUC-tumor-areas corresponded with
high MRT-areas (Fig. 3). 21 days after irradiation both, photon- and 12C-ion-treated
groups, exhibited dose-independently similar values for AUC and MRT,
respectively. For HI-tumors AUC-values remained constant while the MRT of
treated tumors elongated slightly upon 7 days after treatment (Fig. 2b,d).
Pharmacokinetic analysis with ETM showed a decrease in the transfer
constant Ktrans for
AT1-control-tumors while 12C-ion-treated tumors exhibited increasing
Ktrans (Fig. 4a). Photon-treated
AT1-tumors only exhibited small changes in Ktrans.
HI-tumors showed less response: Ktrans-values
decreased for control- and photon-treated tumors while they remained constant
for 12C-ion-treated tumors (Fig. 4b). The plasma volume fraction vp, was elevated for 12C-ion-treated
AT1-tumors at day 21. The interstitial volume ve, remained constant for AT1-control-tumors and showed
an increase for photon and 12C-ion-treated tumors. For the HI-tumors
an overall increase in vp
was observed 3 days after treatment which increased further for 12C-ion-treated
tumors and returned to initial values for the control and photon-treated
tumors. Comparable course of parameters was observed for ve. 21 days after treatment all fit parameters exhibited
maxima for 12C-ion-treated tumors.
Stainings for CD31 and smooth muscle actin (SMA) revealed that irradiated AT1-tumors exhibited
less but CD31+/SMA+ co-expressing vessels compared to
control-tumors with a majority of small C31+/SMA- capillaries
21 days after treatment (Fig 5) 6. At the end point, HI-tumors exhibited overall
larger vessels with less SMA and decreased number of vessels compared to
controls.
Discussion and conclusion
Low AUC- and high MRT-values in AT1-control-tumors indicate necrotic parts
in the centers of the fast growing tumors induced by immature capillaries. At
the same time, PKM reveals increased permeability/flow of remaining vessels in
the 12C-ion-treated AT1-tumors indicated by enhanced Ktrans-values. HI-tumors
showed overall fewer differences with respect to irradiation modality and dose
during the 21 days observation period. Constant AUC-values and a mild
elongation of MRT indicate only minor changes in tumor vasculature after treatment.
For isodose experiments, 12C-ion-treated tumors exhibited larger changes
in ETM-fit parameters indicating a stronger effect of 12C-ion-RT on
tumor vasculature 7. For both tumor sublines, increased ve-values
reflect the increasing stromal part of the tumors due to irradiation induced
cell death.
Due to the AT1-tumor’s poor vascularization the ETM was chosen for
pharmacokinetic analysis 8. One drawback of the ETM is the ambiguity of the parameter Ktrans which reflects both plasma
flow and the capillary permeability. Due to different morphology in HI-tumors a
different PK model might be more suitable (e.g. two compartment exchange model)
to reveal radiation-induced changes in tissue perfusion.
DCE-MRI allows characterization of permeability changes in tumors after irradiation.
Isodose and isoeffective treatments further indicate that beam modality has a stronger
impact on perfusion and permeability for AT1- than for HI-tumors.
Acknowledgements
This work
was supported by the German Research Foundation (DFG, KFO 214, GL 893/1-1 and
KA2679/3-1). The authors are grateful to
the staff of the Heidelberg Ion Therapy Center (HIT) for providing excellent
working conditions.
References
1. Uhl M, Herfarth K, Debus J, Comparing the use of protons and carbon ions
for treatment. The Cancer Journal, 2014;20(6): 433 - 439.
2. Glowa
C, Karger C, Brons S, et al., Carbon ion radiotherapy
decreases the impact of tumor heterogeneity on radiation response in
experimental prostate tumors. Cancer Lett, 2016;378(2): 97-103.
3. Isaacs J, Heston W, Weissman R, Coffey D, Animal model of the hormone-sensitive and
-insensitive prostatic adenocarcinomas, Dunning R-3327-H, R3327-HI, and
R3327-AT1. American Association for Cancer Research, 1978;38: 4353 - 4359.
4. Nolden
M, Zelzer S, Seitel A, et al., The Medical Imaging
Interaction Toolkit: challenges and advances. International Journal of
Computer Assisted Radiology and Surgery, 2013;8(4): 607-620.
5. Sourbron S and Buckley D, Classic models for
dynamic contrast-enhanced MRI. NMR Biomed, 2013;26(8): 1004-27.
6. Glowa
C, In vivo Untersuchungen zur
Wirksamkeit von Bestrahlungen mit Kohlenstoffionen am syngenen Prostatakarzinom
Modell R3327, PhD Thesis 2013, University of Heidelberg.
7. Glowa
C, Peschke P, Brons S, et al., Carbon ion radiotherapy: impact of tumor
differentiation on local control in experimental prostate carcinomas.
Radiation Oncology, 2017; accepted
for publication DOI:10.1186/s13014-017-0914-9.
8. Sourbron
S and Buckley D, On the scope and
interpretation of the Tofts models for DCE-MRI. Magn Reson Med, 2011;66(3): 735-45.