Previous work has shown that hyperpolarized [1,4-13C2]fumarate is a probe of cellular necrosis. We demonstrate here that the ratio of cardiac hyperpolarized malate to fumarate is increased by a factor of $$$\sim$$$82 one day after cryoinduced myocardial infarction in rats, decreasing to an $$$\sim$$$30-fold increase one week after injury. We additionally image this injury with a novel spiral multiband pulse sequence. Hyperpolarized fumarate therefore forms a sensitive probe of myocardial injury in vivo, and could form a clinical monitor of cellular damage and necrosis after infarction.
Hyperpolarization: [1,4-13C2]fumaric acid ($$$3.23\,\text{mmol}$$$; Cambridge Isotopes) was dissolved in $$$8.74\,\text{mmol}$$$ of DMSO containing $$$11.48\,\mu\text{mol}$$$ of a trityl radical (AH111501; GE Healthcare) and $$$0.48\,\mu\text{mol}$$$ of a gadolinium chelate (Dotarem, Guerbet). A $$$40\,\text{mg}$$$ aliquot was polarized per experiment (prototype hyperpolarizer, $$$45\,\text{min}$$$ at $$$94\,\text{GHz}$$$) before dissolution (in $$$6\,\text{ml}$$$ NaOH, final concentration $$$20\,\text{mM}$$$). Infusion ($$$2\,\text{ml}$$$) was via a tail vein cannula over $$$20\,\text{s}$$$ following dissolution
Myocardial Infarction: Six female Wistar rats ($$$\sim200\,\text{g}$$$, Harlan) were divided into two groups (MI or control, $$$n=3$$$), and subject to cryoinduced myocardial infarction.[4] Control animals were subject only to pericardial removal. Pre-operative and postoperative analgesia was provided. All experiments were performed with appropriate ethical review.
Spectroscopy: An actively detuned transmit/surface receive coil was used (72 mm 1H/13C proton/carbon birdcage transmit with $$$40\,\text{mm}$$$ two-channel 13C surface receive; Rapid Biomedical GMBH, Rimpar, Germany) as described previously.[5] A $$$5\,\text{M}$$$ 13C-urea phantom was included as a per-animal FA and frequency reference. Slice-selective spectra ($$$200\,\mu\text{s}$$$ gauss, $$$20\,\text{mm}$$$ thick, TR$$$=\sim1\,\text{s}$$$, bandwidth $$$10\,\text{kHz}$$$, FA $$$10^\circ$$$) were acquired from the heart in end-systole. Cardiac function was assessed by CINE.[6] Spectra were summed for $$$60\,\text{s}$$$ following the appearance of the [1,4-13C2]fumarate peak, and quantified with AMARES, with the reported malate:fumarate ratio being that of total visible malate to fumarate.
Multiband Imaging: A hybrid multiband spatial-spectral RF excitation pulse[7] was designed to simultaneously excite [1,4-13C2]fumarate at a $$$4^\circ$$$ FA, and both [1,4-13C2]malate resonances at $$$\sim20^\circ$$$, and a slab thickness of $$$20\,\text{mm}$$$. A multi-echo spiral readout[8] was constructed to maximise the effective number of signal averages over all chemical species in the subsequent reconstruction, with FID acquisition every seventh echo ($$$\text{TE}=2.1,\,3.8,\,5.5,\,7.2,\,8.9,\,10.6,\,12.3$$$ FID $$$2.1\,\text{ms}$$$). The spiral trajectory was designed with a nominal FOV of $$$80\times80\,\text{mm}^2$$$, readout bandwidth of $$$250\,\text{kHz}$$$, TR$$$=1\,\text{RR}$$$ interval, nominal acquisition in-plane resolution $$$2\times2\,\text{mm}^2$$$. The pulse sequence is shown in Fig. 1. The k-space trajectory was predicted using a premeasured gradient impulse response function.[9] The multiecho reconstruction was performed prior to NUFFT[10] ($$$30\,\text{Hz}$$$ Lorentzian filtered; reconstructed resolution $$$5.62\times5.62\,\text{mm}^2$$$; nominal $$$128\times128$$$ matrix). $$$n=1$$$ control and infarcted animals were scanned; other details as above.
The authors would like thank financial support from an EPSRC Doctoral Training Centre Grant and Doctoral Prize Fellowship (refs. EP/J013250/1 and EP/M508111/1) and St. Hugh's College, Oxford. We also acknowledge financial support from the British Heart Foundation (Fellowships FS/10/002/28078 & FS/11/50/29038, Programme Grant RG/11/9/28921).
[1] P. G. Masci, J. Bogaert, Cardiovasc. Diagn. Ther. 2012, 2, 113–27.
[2] F. A. Gallagher, M. I. Kettunen, D.-E. Hu, P. R. Jensen, R. I. ’. Zandt, M. Karlsson, A. Gisselsson, S. K. Nelson, T. H. Witney, S. E. Bohndiek, G. Hansson, T. Peitersen, M. H. Lerche, K. M. Brindle, Proc. Natl. Acad. Sci. U. S. A. 2009, 106, 19801–19806.
[3] M. R. Clatworthy, M. I. Kettunen, D.-E. Hu, R. J. Mathews, T. H. Witney, B. W. C. Kennedy, S. E. Bohndiek, F. A. Gallagher, L. B. Jarvis, K. G. C. Smith, K. M. Brindle, Proc. Natl. Acad. Sci. U. S. A. Aug. 2012, 109, 13374–13379.
[4] E. J. van den Bos, B. M. Mees, M. C. de Waard, R. de Crom, D. J. Duncker, Am J Physiol Hear. Circ Physiol 2005, 289, H1291–300.
[5] J. J. Miller, A. Z. Lau, I. Teh, J. E. Schneider, P. Kinchesh, S. Smart, V. Ball, N. R. Sibson, D. J. Tyler, Magn. Reson. Med. May 2015, 75, 1515–1524.
[6] J. E. Schneider, P. J. Cassidy, C. Lygate, D. J. Tyler, F. Wiesmann, S. M. Grieve, K. Hulbert, K. Clarke, S. Neubauer, J. Magn. Reson. Imaging Dec. 2003, 18, 691–701.
[7] A. Sigfridsson, K. Weiss, L. Wissmann, J. Busch, M. Krajewski, M. Batel, G. Batsios, M. Ernst, S. Kozerke, Magn. Reson. Med. May 2014, DOI 10.1002/mrm.25294.
[8] F. Wiesinger, E. Weidl, M. I. Menzel, M. A. Janich, O. Khegai, S. J. Glaser, A. Haase, M. Schwaiger, R. F. Schulte, Magn. Reson. Med. July 2012, 68, 8–16.
[9] J. H. Duyn, Y. Yang, J. A. Frank, J. W. van der Veen, J. Magn. Reson. May 1998, 132, 150–3.
[10] J. Fessler, B. Sutton, IEEE Trans. Signal Process. Feb. 2003, 51, 560–574.