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. 2019 Jun 21;150(23):234307.
doi: 10.1063/1.5096036.

Effects of glassing matrix deuteration on the relaxation properties of hyperpolarized 13C spins and free radical electrons at cryogenic temperatures

Affiliations

Effects of glassing matrix deuteration on the relaxation properties of hyperpolarized 13C spins and free radical electrons at cryogenic temperatures

Christopher Parish et al. J Chem Phys. .

Abstract

Glassing matrix deuteration could be a beneficial sample preparation method for 13C dynamic nuclear polarization (DNP) when large electron paramagnetic resonance (EPR) width free radicals are used. However, it could yield the opposite DNP effect when samples are doped with small EPR width free radicals. Herein, we have investigated the influence of solvent deuteration on the 13C nuclear and electron relaxation that go along with the effects on 13C DNP intensities at 3.35 T and 1.2 K. For 13C DNP samples doped with trityl OX063, the 13C DNP signals decreased significantly when the protons are replaced by deuterons in glycerol:water or DMSO:water solvents. Meanwhile, the corresponding solid-state 13C T1 relaxation times of trityl OX063-doped samples generally increased upon solvent deuteration. On the other hand, 13C DNP signals improved by a factor of ∼1.5 to 2 upon solvent deuteration of samples doped with 4-oxo-TEMPO. Despite this 13C DNP increase, there were no significant differences recorded in 13C T1 values of TEMPO-doped samples with nondeuterated or fully deuterated glassing matrices. While solvent deuteration appears to have a negligible effect on the electron T1 relaxation of both free radicals, the electron T2 relaxation times of these two free radicals generally increased upon solvent deuteration. These overall results suggest that while the solid-phase 13C DNP signals are dependent upon the changes in total nuclear Zeeman heat capacity, the 13C relaxation effects are related to 2H/1H nuclear spin diffusion-assisted 13C polarization leakage in addition to the dominant paramagnetic relaxation contribution of free radical centers.

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Figures

FIG. 1.
FIG. 1.
Structures of the free radicals and 13C-labeled compound used in this study.
FIG. 2.
FIG. 2.
Effect of glassing solvent deuteration on trityl OX063-doped 13C DNP samples at 3.35 T and 1.2 K: (a) Top: Representative 13C DNP buildup curves for 13C samples with nondeuterated (ND) and fully deuterated (FD) glassing solvents. Bottom: Comparative bar graphs of extrapolated 13C DNP intensities for ND and FD glycerol:H2O or DMSO:H2O glassing solvents. (b) Top: Representative hyperpolarized 13C T1 decay curves for 13C samples with ND and FD solvents. Bottom: Relative bar graphs of 13C T1 values of frozen 13C DNP samples with ND and FD glassing solvents.
FIG. 3.
FIG. 3.
Influence of glassing solvent deuteration on 13C DNP samples doped with 4-oxo-TEMPO free radical: (a) Top: Representative 13C DNP buildup curves for 13C samples with nondeuterated (ND) and fully deuterated (FD) glassing solvents. Bottom: Comparative bar graphs of 13C DNP intensities for ND and FD glycerol:H2O or DMSO:H2O glassing solvents. (b) Top: Representative hyperpolarized 13C T1 decay curves for 13C samples with ND and FD solvents. Bottom: Relative bar graphs of 13C T1 values of frozen 13C DNP samples with ND and FD solvents. Mean values (N = 3) and standard deviations of 13C DNP signals and 13C T1 values are displayed. All these DNP measurements were taken at 3.35 T and 1.2 K.
FIG. 4.
FIG. 4.
W-band EPR measurements of 13C DNP samples: (a) Top: Representative EPR spectra of trityl OX063 with ND and FD glassing solvents. Bottom: Temperature dependence of trityl OX063 electron spin-lattice relaxation rate (1/T1) for 13C DNP samples with ND and FD glycerol:H2O or DMSO:H2O glassing matrices. (b) Top: Representative EPR spectra of 4-oxo-TEMPO in ND and FD solvents. Bottom: 4-Oxo-TEMPO electron T1 relaxation rates vs temperature in ND and FD glassing solvents. The dashed lines denote the apparent temperature power-law dependence of electron 1/T1.
FIG. 5.
FIG. 5.
(a) Representative electron T2 transverse magnetization dephasing curves for trityl OX063 in ND and FD glycerol:water solvents at W-band and 5 K. The solid curves are fits to an exponential decay equation. (b) Bar graphs showing the increase in electron T2 values of trityl OX063 and 4-oxo-TEMPO at W-band and 5 K upon deuteration of the glassing solvents.

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References

    1. Levitt M. H., Spin Dynamics: Basics of Nuclear Magnetic Resonance, 2nd ed. (John Wiley & Sons, Ltd., West Sussex, 2008).
    1. Slichter C. P., Principles of Magnetic Resonance, 3rd ed. (Springer-Verlag, Berlin, 1990).
    1. Abragam A., The Principles of Nuclear Magnetism (Clarendon Press, Oxford, 1961).
    1. Abragam A. and Goldman M., Rep. Prog. Phys. 41, 395 (1978).10.1088/0034-4885/41/3/002 - DOI
    1. Crabb D. G. and Meyer W., Annu. Rev. Nucl. Part. Sci. 47, 67 (1997).10.1146/annurev.nucl.47.1.67 - DOI