Frédéric
Mentink-Vigier
ab,
Anne-Laure
Barra
c,
Johan
van Tol
b,
Sabine
Hediger
a,
Daniel
Lee
a and
Gaël
De Paëpe
*a
aUniv. Grenoble Alpes, CEA, CNRS, INAC-MEM, F-38000 Grenoble, France. E-mail: gael.depaepe@cea.fr
bNational High Magnetic Field Laboratory, Florida State University, Tallahassee, FL 32310, USA
cLaboratoire National des Champs Magnétiques Intenses – CNRS, Univ. Grenoble Alpes, F-38042 Grenoble, France
First published on 11th June 2021
Correction for ‘De novo prediction of cross-effect efficiency for magic angle spinning dynamic nuclear polarization’ by Frédéric Mentink-Vigier et al., Phys. Chem. Chem. Phys., 2019, 21, 2166–2176, DOI: 10.1039/C8CP06819D.
Biradical | g-Tensor [gx, gy, gz] | g-Tensor relative orientation (α, β, γ) | 14N hyperfine coupling (MHz) | Dipolar coupling/J-exchange interaction (MHz) | Dipolar orientation (ϕ, θ) |
---|---|---|---|---|---|
a n.c. = not calculated. | |||||
TEKPol DFT | [2.0094, 2.0070, 2.0024] | [−70.4, 79.7, −63.7] | n.c.a | 30.5/n.c. | [10, 66.3] |
TEKPol Exp. | [2.0095, 2.0060, 2.0021] ± 2 × 10−4 | [−75.4, 79.6, −58.6] ± 2.5 | [18, 16, 98] ± 2 | 30.5 ± 1/−1 ± 1 | [10, 66.3] ± 3 |
AMUPol DFT | [2.0091, 2.0067, 2.0024] | [125.1, 129.7, −46.6] | n.c.a | 34.75/n.c. | [−174.6, 74] |
AMUPol Exp. | [2.0092, 2.0061, 2.0020] ± 2 × 10−4 | [123.1, 129.8, −46] ± [2.5, 5, 2.5] | [18, 17, 100] ± 2 | 35 ± 2/−16 ± 2 | [−174, 76] ± 5 |
A sentence in the conclusion should also be modified to: “it clearly confirms the presence of an exchange interaction of ∼−15 MHz and a dipolar coupling of ∼35 MHz for AMUPol, as initially reported,23,30 although it was a matter of debate78 until recently.68”
In addition, Fig. 4 was incorrect: the grey overlay representing the error was shifted. The corrected figure is shown below.
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Fig. 4 High-field EPR spectrum of 10 mM of AMUPol in D8-glycerol/D2O/H2O (60/30/10 v%) + 2M 13C-urea, recorded at 100 K, for a microwave frequency of 240 GHz. The red curve represents the experimental spectrum and the red dashed line represents the theoretical EPR spectrum obtained with fitted parameters reported in Table 1. The blue dots correspond to the measured electron spin–lattice relaxation times, T1e (right axis). |
The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers.
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