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Correction: De novo prediction of cross-effect efficiency for magic angle spinning dynamic nuclear polarization

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

Received 28th May 2021 , Accepted 28th May 2021

First published on 11th June 2021


Abstract

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.


The authors wish to correct the sign of the J-exchange interaction in Table 1 in order to match the convention defined in the Supporting Information. The J-exchange interaction values are all negative under the convention image file: d1cp90117f-t1.tif. The corrected version of Table 1 is shown below.
Table 1 List of the calculated (DFT) and experimental geometric parameters (after fitting) for the TEKPol and AMUPol biradicals. Euler angles are given in degrees with respect to the first g-tensor, using Easyspin's v 5.1 rotation convention (active rotation).67 The g-strains for the simulations are proportional to ([1.3 × (gx − 2), gy − 2, gz − 2] × 6%) and are [0.8, 0.35, 0.13] × 10−3 for TEKPol and [0.8, 0.3, 0.12] × 10−3 for AMUPol
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.


image file: d1cp90117f-f4.tif
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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