Dynamic nuclear polarisation via the integrated solid effect II: experiments on naphthalene-h8doped with pentacene-d14 #DNPNMR

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Dynamic nuclear polarisation via the integrated solid effect II: experiments on naphthalene-h8doped with pentacene-d14 #DNPNMR

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Eichhorn, T.R., et al., Dynamic nuclear polarisation via the integrated solid effect II: experiments on naphthalene-h8doped with pentacene-d14. Mol. Phys., 2013. 112(13): p. 1773-1782.


https://doi.org/10.1080/00268976.2013.863405


In dynamic nuclear polarisation (DNP), also called hyperpolarisation, a small amount of unpaired electron spins is added to the sample containing the nuclear spins, and the polarisation of these unpaired electron spins is transferred to the nuclear spins by means of a microwave field. Traditional DNP polarises the electron spin of stable paramagnetic centres by cooling down to low temperature and applying a strong magnetic field. Then weak continuous wave microwave fields are used to induce the polarisation transfer. Complicated cryogenic equipment and strong magnets can be avoided using short-lived photo-excited triplet states that are strongly aligned in the optical excitation process. However, a much faster transfer of the electron spin polarisation is needed and pulsed DNP methods like nuclear orientation via electron spin locking (NOVEL) and the integrated solid effect (ISE) are used. To describe the polarisation transfer with the strong microwave fields in NOVEL and ISE, the usual perturbation methods cannot be used anymore. In the previous paper, we presented a theoretical approach to calculate the polarisation transfer in ISE. In the present paper, the theory is applied to the system naphthalene-h8 doped with pentacene-d14 yielding the photo-excited triplet states and compared with experimental results.
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