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. 2018 Mar 1;9(5):1112-1117.
doi: 10.1021/acs.jpclett.7b03026. Epub 2018 Feb 19.

SABRE-Relay: A Versatile Route to Hyperpolarization

Affiliations

SABRE-Relay: A Versatile Route to Hyperpolarization

Soumya S Roy et al. J Phys Chem Lett. .

Abstract

Signal Amplification by Reversible Exchange (SABRE) is used to switch on the latent singlet spin order of para-hydrogen (p-H2) so that it can hyperpolarize a substrate (sub = nicotinamide, nicotinate, niacin, pyrimidine, and pyrazine). The substrate then reacts reversibly with [Pt(OTf)2(bis-diphenylphosphinopropane)] by displacing OTf- to form [Pt(OTf)(sub)(bis-diphenylphosphinopropane)]OTf. The 31P NMR signals of these metal complexes prove to be enhanced when the substrate possesses an accessible singlet state or long-lived Zeeman polarization. In the case of pyrazine, the corresponding 31P signal was 105 ± 8 times larger than expected, which equated to an 8 h reduction in total scan time for an equivalent signal-to-noise ratio under normal acquisition conditions. Hence, p-H2 derived spin order is successfully relayed into a second metal complex via a suitable polarization carrier (sub). When fully developed, we expect this route involving a second catalyst to successfully hyperpolarize many classes of substrates that are not amenable to the original SABRE method.

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Conflict of interest statement

The authors declare no competing financial interest.

Figures

Scheme 1
Scheme 1. Schematic Depiction of the SABRE-Relay
Substrate S1 binds reversibly alongside p-H2 to metal complex M1 and becomes hyperpolarized. S1 then binds reversibly to M2–S1 and polarization is relayed into its 31P response.
Scheme 2
Scheme 2. Identities of S1 Used in This SABRE-Relay Study
Scheme 3
Scheme 3. Relayed Transfer of Polarization from p-H2 into a Second Agent
Precatalyst [IrCl(IMes)(COD)] (M1) is transformed into [Ir(H)2(IMes)(S1)3]Cl (M1–S1) by adding p-H2 gas and substrate S1. S1 then gains hyperpolarized Zeeman and singlet spin order via polarization transfer from p-H2 depending on its identity. In a second step, the 31P response of M2–S1 becomes hyperpolarized.
Figure 1
Figure 1
Experimental scheme for SABRE-Relay, showing timings, magnetic field variance, and rf sequence. First, the sample is mixed with enriched p-H2 at low magnetic field (∼6 mT and ∼1–10 μT) for the durations of τLF1 and τLF2 before moving to high field (τtr) for NMR observation. A simultaneous 90° pulse is applied to 1H and 31P prior to acquiring the 31P signal with 1H decoupling (protocol 1). In a second variant, protocol 2, an M2S sequence, is applied between τLF1 and τLF2.
Figure 2
Figure 2
Single-scan 31P{1H} NMR spectra associated with (A) M2–S1a, (B) M2–S1b, (C) M2–S1c, and (D) M2–S1d using SABRE-Relay protocol 1 of Figure 1.
Figure 3
Figure 3
31P{1H} NMR spectra associated with M2–S1g and M2–S1h (structures above the NMR spectra) that form from M2 and S1g or S1h, respectively. In both cases, the upper 31P NMR spectrum is the control, which involved 128 transients, while the lower NMR spectrum was acquired by SABRE-Relay through process 1 and associated with a single detection pulse according to Figure 2.

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