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Dynamic nuclear polarization of ¹³C nuclei in the liquid state over a 10 Tesla field range.

MPS-Authors
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Orlando,  T.
Research Group of Electron Paramagnetic Resonance, MPI for Biophysical Chemistry, Max Planck Society;

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Dervisoglu,  R.
Research Group of Solid State NMR Spectroscopy-2, MPI for Biophysical Chemistry, Max Planck Society;

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Levien,  M.
Research Group of Electron Paramagnetic Resonance, MPI for Biophysical Chemistry, Max Planck Society;

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Tkach,  I.
Research Group of Electron Paramagnetic Resonance, MPI for Biophysical Chemistry, Max Planck Society;

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Andreas,  L.
Research Group of Solid State NMR Spectroscopy-2, MPI for Biophysical Chemistry, Max Planck Society;

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Bennati,  M.
Research Group of Electron Paramagnetic Resonance, MPI for Biophysical Chemistry, Max Planck Society;

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3011432_Suppl.pdf
(Supplementary material), 9MB

Citation

Orlando, T., Dervisoglu, R., Levien, M., Tkach, I., Prisner, T. F., Andreas, L., et al. (2019). Dynamic nuclear polarization of ¹³C nuclei in the liquid state over a 10 Tesla field range. Angewandte Chemie International Edition, 58(5), 1402-1406. doi:10.1002/anie.201811892.


Cite as: http://hdl.handle.net/21.11116/0000-0002-9852-6
Abstract
Nuclear magnetic resonance (NMR) techniques play an essential role in natural science and medicine. In spite of the tremendous utility associated with the small energies detected, the most severe limitation is the low signal-to-noise ratio. Dynamic nuclear polarization (DNP), a technique based on transfer of polarization from electron to nuclear spins, has emerged as a tool to enhance sensitivity of NMR. However, the approach in liquids is still facing several challenges. Here we report the observation of room temperature, liquid DNP ¹³C signal enhancements in organic small molecules as high as 600 at 9.4 Tesla and 800 at 1.2 Tesla. A mechanistic investigation of the ¹³C-DNP field dependence shines light on parameters governing the underlying scalar DNP, indicating that DNP efficiency is raised by proper choice of the polarizing agent (paramagnetic center) and by halogen atoms as mediators of scalar hyperfine interaction. Observation of sizable DNP of ¹³CH₂ and ¹³CH₃ groups in organic molecules at 9.4 T opens up perspective for a broader application of this method .