“…Magnetic resonance imaging (MRI) is ubiquitous in laboratories and in our daily life,w ith applications ranging from chemical engineering (measurement of molecular diffusion, dispersion, and flow hydrodynamics within reactors [1] or probing of catalysts [2,3] and catalytic processes from the nanometer-to-centimeter scale) to in vivo MRI of tissues or target organs,w ithout the need for damaging radiation. However,N MR (or MRI) suffers from an intrinsically low sensitivity,a rising from the low thermal equilibrium (Boltzmann) polarization of the nuclear spins at room temperature, even with the highest-field instruments.This drawback can be circumvented by dynamic nuclear polarization (DNP), which allows for dramatic NMR signal enhancements well beyond thermal equilibrium at low temperatures by microwaveinduced cross-polarization from highly thermally polarized electron spins to nuclear spins.B ased on this DNP phenomenon, dissolution DNP (d-DNP) setups have been developed since 2003 to polarize as ample at low temperature (1-4 K), astep which is then followed by rapid dissolution to the liquid state;the hyperpolarized solution is then transferred from the polarizer to an NMR spectrometer or MRI scanner.…”