Abstract

This work explores the dynamic nuclear polarization (DNP) of 1H and 19F nuclei in a sample of 25/75 (% v/v) fluorobenzene/toluene containing the radical 1,3-bisphenylene-2-phenylallyl radical (BDPA) as a polarizing agent. Previously, heteronuclear effects in DNP were studied by analysing the shapes of DNP spectra, or by observing cross-relaxation between nuclei of different types. In this work, we report a rather specific DNP spectrum, where 1H and 19F nuclei obtain polarizations of opposite signs upon microwave (MW) irradiation. In order to explain this observation, we introduce a novel mechanism called heteronuclear thermal mixing (hn-TM). Within this mechanism the spectra of opposite signs can then be explained due to the presence of four-spin systems, involving a pair of dipolar coupled electron spins and hyperfine coupled nuclear spins of 1H and 19F, such that a condition relating their Larmor frequencies |ω1e - ω2e| ≈ ωH - ωF is satisfied. Under this condition, a strong mixing of electron and nuclear states takes place, enabling simultaneous four-spin flip-flops. Irradiation of electron spin transitions with MW followed by such four-spin flip-flops produces non-equilibrium populations of |αHβF and |βHαF states, thus leading to the enhancements of opposite signs for 1H and 19F. Signal enhancements, build-up times and DNP-spectra as a function of MW power and polarizing agent concentration, all provide additional support for assigning the observed DNP mechanism as hn-TM and distinguishing it from other possible mechanisms. We also develop a quantum mechanical model of hn-TM based on averaging of spin Hamiltonians. Simulations based on this model show very good qualitative agreement with experimental data. In addition, the system exhibits cross-relaxation between 1H and 19F induced by the presence of BDPA, which was detected by measuring the 19F signal build-up upon saturation of 1H nuclei with a train of radio-frequency pulses. We demonstrate that such cross-relaxation most likely originates due to the same electron and nuclear states mixing in the four-spin systems.

Highlights

  • Dynamic Nuclear Polarization (DNP) allows increasing the nuclear magnetic resonance (NMR) signals by transferring large polarization of electron spins onto coupled nuclear spins via microwave (MW) irradiation

  • The observed characteristic 1H and 19F-DNP spectra arising due to heteronuclear DNP (hn-DNP) were explained using a hn-thermal mixing (TM) mechanism, which is based on the presence of electron and nuclear states mixing in a four-spin system

  • The characteristic DNP spectrum arising due to hn-DNP involving 19F and 1H becomes distinguishable from the DNP spectra due to other mechanisms, because of a small difference of nuclear Larmor frequencies, a rather narrow linewidth of BDPA and a small contribution of a regular thermal mixing of 1H and 19F to the DNP spectrum

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Summary

Introduction

Dynamic Nuclear Polarization (DNP) allows increasing the nuclear magnetic resonance (NMR) signals by transferring large polarization of electron spins onto coupled nuclear spins via microwave (MW) irradiation. Signal enhancements due to DNP are widely used to improve the sensitivity of solid state and solution NMR spectroscopy[1,2], as well as medical magnetic resonance imaging[3]. In many of these applications, the studied samples contain more than one type of polarizable nuclei, further referred to as heteronuclei. In systems with heteronuclei the presence of unpaired electrons induces a polarization exchange between nuclei of different types, thereby indirectly affecting the dynamics of their polarization build-up in the DNP experiments.

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