Nuclear spin hyperpolarization techniques are revolutionizing the field of 13C molecular MRI. While dissolution dynamic nuclear polarization (d‐DNP) is currently the leading technique, it is generally slow (requiring ≈1 h) and costly (≈$USD106). As a consequence of carbon's central place in biochemistry, tremendous progress using 13C d‐DNP bioimaging has been demonstrated to date including a number of clinical trials. Despite numerous attempts to develop alternatives to d‐DNP, the competing methods have faced significant translational challenges. Efficient hyperpolarization of 15N, 31P, and other heteronuclei using signal amplification by reversible exchange (SABRE) has been reported in 2015, but extension of this technique to 13C has proven to be challenging. Here, we present efficient hyperpolarization of 13C nuclei using micro‐Tesla SABRE. Up to ca. 6700‐fold enhancement of nuclear spin polarization at 8.45 T is achieved within seconds, corresponding to P13C ≈4.4 % using 50 % parahydrogen (P13C >14 % would be feasible using more potent ≈100 % parahydrogen). Importantly, the 13C polarization achieved via SABRE strongly depends not only upon spin–lattice relaxation, but also upon the presence of 15N (I=1/2) versus quadrupolar 14N (I=1) spins in the site binding the hexacoordinate Ir atom of the catalytic complex. We show that different 13C nuclei in the test molecular frameworks—pyridine and acetonitrile—can be hyperpolarized, including 13C sites up to five chemical bonds away from the exchangeable hydrides. The presented approach is highly scalable and can be applied to a rapidly growing number of biomolecules amendable to micro‐Tesla SABRE.
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Barskiy et al. (2017) studied this question.
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