LIGHT-SABRE Hyperpolarizes 1- 13 C-Pyruvate Continuously without Magnetic Field Cycling

Nuclear spin hyperpolarization enables real-time observation of metabolism and intermolecular interactions . 1- C-pyruvate is the leading hyperpolarized tracer currently under evaluation in several clinical trials as a promising molecular imaging agent. Still, the quest for a simple, fast, and effic...

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Veröffentlicht in:Journal of physical chemistry. C 2023-04, Vol.127 (14), p.6744-6753
Hauptverfasser: Pravdivtsev, Andrey N, Buckenmaier, Kai, Kempf, Nicolas, Stevanato, Gabriele, Scheffler, Klaus, Engelmann, Joern, Plaumann, Markus, Koerber, Rainer, Hövener, Jan-Bernd, Theis, Thomas
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Sprache:eng
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Zusammenfassung:Nuclear spin hyperpolarization enables real-time observation of metabolism and intermolecular interactions . 1- C-pyruvate is the leading hyperpolarized tracer currently under evaluation in several clinical trials as a promising molecular imaging agent. Still, the quest for a simple, fast, and efficient hyperpolarization technique is ongoing. Here, we describe that continuous, weak irradiation in the audio-frequency range of the C spin at the 121 μT magnetic field (approximately twice Earth's field) enables spin order transfer from parahydrogen to C magnetization of 1- C-pyruvate. These so-called LIGHT-SABRE pulses couple nuclear spin states of parahydrogen and pyruvate via the -coupling network of reversibly exchanging Ir-complexes. Using ∼100% parahydrogen at ambient pressure, we polarized 51 mM 1- C-pyruvate in the presence of 5.1 mM Ir-complex continuously and repeatedly to a polarization of 1.1% averaged over free and catalyst-bound pyruvate. The experiments were conducted at -8 °C, where almost exclusively bound pyruvate was observed, corresponding to an estimated 11% polarization on bound pyruvate. The obtained hyperpolarization levels closely match those obtained via SABRE-SHEATH under otherwise identical conditions. The creation of three different types of spin orders was observed: transverse C magnetization along the applied magnetic field, C -magnetization along the main field , and C- H -spin order. With a superconducting quantum interference device (SQUID) for detection, we found that the generated spin orders result from H- C -coupling interactions, which are not visible even with our narrow linewidth below 0.3 Hz and at -8 °C.
ISSN:1932-7447
1932-7455
DOI:10.1021/acs.jpcc.3c01128