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. 2019 Jan 23;10:395. doi: 10.1038/s41467-019-08298-8

Fig. 2.

Fig. 2

Coherent hyperpolarization experiments. a DARTH_SABRE pulse sequence, where DARTH-pulses of length τp are given at intervals of τd for “n” repetitions and applied to the bound 15N spin slightly off-resonance. The pulses adiabatically ramp towards the optimal matching condition to induce higher polarizations. b Coherent SHEATH pulse sequence, where analogous pulses are delivered to the sample at the optimal field condition, which is typically ≈0.5 μT, with inter-pulse delays using a ≈55 μT field to store magnetization. c Experimental DARTH-SABRE dynamics of an AA’XX’ spin system using 50 mM 15N-pyridine with an inter-pulse delay of τd=600 μs at 8.45 T. d Experimental coherent SHEATH dynamics of an AA’X spin system using 100 mM 15N-benzonitrile with 33 mM pyridine and an inter-pulse delay of τd = 350 ms; detection was performed at 8.45 T. Data are shown fit to numerical QMC simulations using average PTC lifetimes of 20 ms (DARTH) and 50 ms (SHEATH). e Polarization as a function of the delay parameter for the DARTH-SABRE sequence using a 25 ms DARTH pulse, which corresponds to a π pulse. f Evolution of singlet population excess (DARTH AA’XX’: SH0TH0, blue line; SHEATH AA’X: SH0–TH-, red line) under the conditions used in the fit of the experimental data and normalized to the initial SH0 population