Literature DB >> 21258686

Determination of the temperature dependence of the dynamic nuclear polarisation enhancement of water protons at 3.4 Tesla.

Eugeny V Kryukov1, Kevin J Pike, Thomas K Y Tam, Mark E Newton, Mark E Smith, Ray Dupree.   

Abstract

It is shown that the temperature dependence of the DNP enhancement of the NMR signal from water protons at 3.4 T using TEMPOL as a polarising agent can be obtained provided that the nuclear relaxation, T(1I), is sufficiently fast and the resolution sufficient to measure the (1)H NMR shift. For high radical concentrations (∼100 mM) the leakage factor is approximately 1 and, provided sufficient microwave power is available, the saturation factor is also approximately 1. In this situation the DNP enhancement is solely a product of the ratio of the electron and nuclear gyromagnetic ratios and the coupling factor enabling the latter to be directly determined. Although the use of high microwave power levels needed to ensure saturation causes rapid heating of the sample, this does not prevent maximum DNP enhancements, ε(0), being obtained since T(1I) is very much less than the characteristic heating time at these concentrations. It is necessary, however, to know the temperature variation of T(1I) to allow accurate modelling of the behaviour. The DNP enhancement is found to vary linearly with temperature with ε(0)(T) = -2 ± 2 - (1.35 ± 0.02)T for 6 °C ≤ T ≤ 100 °C. The value determined for the coupling factor, 0.055 ± 0.003 at 25 °C, agrees very well with the molecular dynamics simulations of Sezer et al. (Phys. Chem. Chem. Phys., 2009, 11, 6626) who calculated 0.0534, however the experimental values increase much more rapidly with increasing temperature than predicted by these simulations. Large DNP enhancements (|ε(0)| > 100) are reported at high temperatures but it is also shown that significant enhancements (e.g.∼40) can be achieved whilst maintaining the sample temperature at 40 °C by adjusting the microwave power and irradiation time. In addition, short polarisation times enable rapid data acquisition which permits further enhancement of the signal, such that useful liquid state DNP-NMR experiments could be carried out on very small samples.

Entities:  

Year:  2011        PMID: 21258686     DOI: 10.1039/c0cp02188a

Source DB:  PubMed          Journal:  Phys Chem Chem Phys        ISSN: 1463-9076            Impact factor:   3.676


  4 in total

1.  Comparison of Overhauser DNP at 0.34 and 3.4 T with Frémy's Salt.

Authors:  M-T Türke; M Bennati
Journal:  Appl Magn Reson       Date:  2012-06-03       Impact factor: 0.831

2.  The influence of Ho3+ doping on 13C DNP in the presence of BDPA.

Authors:  Ram B Khattri; Ali A Sirusi; Eul Hyun Suh; Zoltan Kovacs; Matthew E Merritt
Journal:  Phys Chem Chem Phys       Date:  2019-08-28       Impact factor: 3.676

3.  High-resolution Overhauser dynamic nuclear polarization enhanced proton NMR spectroscopy at low magnetic fields.

Authors:  Timothy J Keller; Alexander J Laut; Jagadishwar Sirigiri; Thorsten Maly
Journal:  J Magn Reson       Date:  2020-03-18       Impact factor: 2.229

4.  Optimization and prediction of the electron-nuclear dipolar and scalar interaction in 1H and 13C liquid state dynamic nuclear polarization.

Authors:  X Wang; W C Isley Iii; S I Salido; Z Sun; L Song; K H Tsai; C J Cramer; H C Dorn
Journal:  Chem Sci       Date:  2015-07-29       Impact factor: 9.825

  4 in total

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