31P spectroscopic imaging for evaluation of early effects of photodynamic treatment on tumor metabolism
Tom Schreurs1, Sophie Peereboom2, Gustav Strijkers3, Jeanine Prompers1, and Klaas Nicolay1

1Biomedical Engineering, Eindhoven University of Technology, Eindhoven, Netherlands, 2Biomedical Engineering, ETH Zürich, Zürich, Switzerland, 3Bioengineering and Physics, Academic Medical Center Amsterdam, Amsterdam, Netherlands

Synopsis

The feasibility of 31P spectroscopic imaging to evaluate effects of photodynamic therapy (PDT) on tumor metabolism was assessed. In PDT, a light-activated drug and local laser irradiation are used to ablate tumors. Spectroscopic imaging was used to visualize ATP and Pi after PDT in a mouse tumor model before, during, and up to 1 day after PDT. Treatment was performed inside the 9.4T scanner. Clear changes in phosphorus metabolite signals were already observed at 20 min after PDT, indicating a rapid decrease in energetic status. Moreover, the potential of spectroscopic imaging to detect spatial heterogeneities in these changes was demonstrated.

Introduction

In this work, we investigated the feasibility of using 31P spectroscopic imaging to evaluate the early effects of photodynamic therapy (PDT) on tumor metabolism. PDT is an emerging cancer treatment modality [1], which relies on a light-activated drug that generates cytotoxic oxygen radicals upon local illumination. The primary biological actions are 1) direct cell death and 2) vascular shutdown. While PDT has proven clinically successful in a range of superficial cancer types, there is a need for early evaluation methods of treatment outcome. Moreover, development of new PDT drugs and optimization of treatment protocols requires techniques to assess PDT efficacy. Since mitochondria are a known target of many photosensitizers, PDT may affect tissue energy metabolism, resulting in lower adenosine triphosphate (ATP) levels. It has been shown that 31P MRS allows rapid detection of PDT-induced changes in phosphorus metabolites, but only with surface coil localization [2]. Here, we assessed the feasibility of using 31P spectroscopic imaging to evaluate the early effects of PDT on tumor metabolism in a spatially resolved manner.

Materials and methods

Eight Balb/C mice with s.c. CT26 colon carcinoma tumors were examined when tumors were 258 +/- 71 mm3. PDT-treated mice (n=6) received an i.v. injection of the photosensitizer Bremachlorin, followed 6 h later by 10 min irradiation with a 655 nm laser at 200 mW/cm2. Light was delivered inside the scanner with a custom-built optic setup, creating a Ø10 mm parallel beam, which was aimed onto the tumor (Figure 1). Controls (n=2) received no photosensitizer or light. MRI was performed with a 9.4 T small animal scanner (Bruker BioSpec), using a volume coil for Tx/Rx of proton signals and transmission of 31P RF pulses. A 31P surface coil was positioned on the tumor for signal reception. T2w anatomical reference images were first acquired. Next, a 31P Chemical Shift Imaging (CSI) baseline scan was obtained in 40 min, in a 5 mm central axial tumor slice. A series of five 10 min Image Selected In vivo Spectroscopy (ISIS) scans was acquired in an as large as possible single voxel within the tumor, to detect immediate changes. PDT was performed during the 2nd ISIS scan. Finally, another CSI scan was acquired. 24h later, single ISIS and CSI scans were obtained. Afterwards, tumors were excised and stored for histological analysis. For both ISIS and CSI, a 1.2 ms sinc-shaped excitation pulse was used, spectral BW = 5000 Hz, γ-ATP was put on resonance, and local shimming was performed. ISIS-specific parameters: 6.25 ms adiabatic hyperbolic secant inversion pulses, FA = 90°, TR = 2 s. CSI specific parameters: 24 mm FOV, 8x8 matrix, Hanning weighted k-space acquisition, FA = 35°, TR = 366 ms. 31P spectra were analyzed in jMRUI. The AMARES algorithm [3] was used to fit the following peaks: inorganic phosphate (Pi), γ-ATP (doublet), α-ATP (double), β-ATP (triplet), phosphocreatine, and phosphomonoesters (PME). Metabolite levels were expressed relative to the total 31P signal in the spectrum.

Results

For all mice, the baseline ISIS tumor spectrum contained a distinct Pi peak (Figure 2). PME and γ-, β-, and α-ATP could generally also be distinguished, but with lower SNR. In contrast to controls, PDT resulted in a significant increase in P­i within 20 minutes after treatment (Figure 3). Moreover, ATP levels decreased after PDT treatment, although this did not reach statistical significance. The observed changes can be attributed to decreased mitochondrial production of ATP, while P­i probably accumulated as the end-product of sustained ATP consumption. Metabolite maps with 3 mm spatial resolution could be calculated from CSI data, which allowed clear spatial and spectral distinction between muscle and tumor tissue (Figure 4). PDT-induced increases in Pi were observed in CSI measurements, homogeneously within the tumor, while Pi levels did not change in controls (Figure 5). We are currently performing extensive histological validation. Based on histological findings from previous studies with the same treatment protocol, treated tumors are generally entirely non-viable at 24h after PDT [4]. This is in line with our current observations of a severely impaired tumor energetic status.

Discussion and Conclusion

Using 31P MRS, we have shown that changes in tumor energy metabolism can be detected within tens of minutes after PDT in our animal model. Moreover, 31P spectroscopic imaging allows for detection of spatial heterogeneity in treatment response, which was not observed with the current treatment protocol, however. This 31P MRS method can be useful for mechanistic PDT research, optimization of PDT drugs or treatment protocols, but might also be clinically valuable for early prediction of treatment outcome.

Acknowledgements

This work is supported by NanoNextNL, a micro and nanotechnology consortium of the Government of the Netherlands and 130 partners

References

1) Agostinis et al., CA Cancer J. Clin. 61: 250-281, 2011
2) Ceckler et al., Biochem. Biophys. Res. Commun. 140 (1): 273-9, 1986
3) Vanhamme et al. J. Magn. Reson. 129 (1): 35-43, 1997
4) Schreurs et al., Proc. of the 23rd Ann. Meeting of ISMRM. Toronto, 2015: 3857

Figures

Setup for PDT treatment during MRI. The 31P surface coil is positioned on the tumor. The bottom picture also shows a tube, containing a collimating lens. The prism attached to the tube directs the light onto the tumor. Mouse heating pad and rectal temperature are not shown.

Typical ISIS spectra before, during and after PDT. γ-ATP was put at 0 ppm. Note the increasing amplitude of the P­i peak after PDT, especially 24h post. Moreover, the ATP peaks have almost completely vanished after 24h.

ISIS peak amplitudes, normalized to P­total, as a function of time for treated animals (n=5) and controls (n=2). The average Pi significantly increased 20 min and 1 day post PDT compared with baseline (both paired t-tests, p < 0.05). The average sum of all ATP peaks decreased, although statistically insignificant.

Tumor and muscle can be distinguished in the anatomical reference image (top left). PCr and Pi fitted amplitude maps calculated from CSI data are shown as green and red overlays, respectively (bottom left). Tumor and muscle pixel spectra (right), contain distinct Pi and PCr peaks, respectively, and ATP.

Typical examples of CSI maps of Pi / Ptotal peak ratios from a control animal and a treated animal. Pi clearly increased in the treated tumor after 40 min, and even more distinctly after 24h. For the control animal, no changes were observed.



Proc. Intl. Soc. Mag. Reson. Med. 24 (2016)
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