TY - JOUR
T1 - Proton hyperfine couplings and Overhauser DNP
AU - Mardini, Michael
AU - George, Christy
AU - Palani, Ravi Shankar
AU - Du, Xizi
AU - Tan, Kong Ooi
AU - Sergeyev, Ivan
AU - Liu, Yangping
AU - Griffin, Robert G.
N1 - Publisher Copyright:
© 2024 Elsevier Inc.
PY - 2024/12
Y1 - 2024/12
N2 - We have prepared trityl radicals with protons at the positions of the -COOH group in the phenyl rings and examined their EPR spectra, which show large [Formula presented] - [Formula presented] hyperfine couplings, and their dynamic nuclear polarization (DNP) Zeeman field profiles. By assessing these polarizing agents for high-field and Overhauser effect DNP, we gain insight into the roles that these hyperfine couplings and other molecular properties play in the DNP performance of these radicals. Interestingly, we do not observe OE DNP in any of the three molecules we examined. This suggests that hyperfine couplings by themselves are not sufficient to support OE DNP. In this case the electron spin density is ∼75 % localized on the central carbon atom rather than being distributed uniformly over the aromatic rings. This is in contrast to BDPA where the distribution is delocalized. Our findings do not suggest that any of these radicals are particularly well-suited to high-field DNP. Furthermore, we emphasize that polarizing agents can be extremely sensitive to their solvent environment, even obscuring the intrinsic magnetic properties of the radical.
AB - We have prepared trityl radicals with protons at the positions of the -COOH group in the phenyl rings and examined their EPR spectra, which show large [Formula presented] - [Formula presented] hyperfine couplings, and their dynamic nuclear polarization (DNP) Zeeman field profiles. By assessing these polarizing agents for high-field and Overhauser effect DNP, we gain insight into the roles that these hyperfine couplings and other molecular properties play in the DNP performance of these radicals. Interestingly, we do not observe OE DNP in any of the three molecules we examined. This suggests that hyperfine couplings by themselves are not sufficient to support OE DNP. In this case the electron spin density is ∼75 % localized on the central carbon atom rather than being distributed uniformly over the aromatic rings. This is in contrast to BDPA where the distribution is delocalized. Our findings do not suggest that any of these radicals are particularly well-suited to high-field DNP. Furthermore, we emphasize that polarizing agents can be extremely sensitive to their solvent environment, even obscuring the intrinsic magnetic properties of the radical.
UR - https://www.scopus.com/pages/publications/85209560713
UR - https://www.scopus.com/pages/publications/85209560713#tab=citedBy
U2 - 10.1016/j.jmr.2024.107797
DO - 10.1016/j.jmr.2024.107797
M3 - Article
C2 - 39566367
AN - SCOPUS:85209560713
SN - 1090-7807
VL - 369
JO - Journal of Magnetic Resonance
JF - Journal of Magnetic Resonance
M1 - 107797
ER -