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Correction: Anisotropy of the vorticity tensor as a magnetic indicator of aromaticity

S. Pelloni a and P. Lazzeretti *b
aIstituto d'istruzione superiore Francesco Selmi, via Leonardo da Vinci, 300, 41126 Modena, Italy
bIstituto di Struttura della Materia, Consiglio Nazionale delle Ricerche, Via del Fosso del Cavaliere 100, 00133 Roma, Italy. E-mail: lazzeret@gmail.com

Received 28th April 2020 , Accepted 28th April 2020

First published on 13th May 2020


Abstract

Correction for ‘Anisotropy of the vorticity tensor as a magnetic indicator of aromaticity’ by S. Pelloni et al., Phys. Chem. Chem. Phys., 2020, 22, 1299–1305, DOI: 10.1039/C9CP05563K.


An error was detected,1 and is hereby corrected, in the computation of the paramagnetic contribution to the vorticity tensor, correctly defined by eqn (15) in the published article. The computer code was incorrect by a factor of −2, which caused an overestimation of its magnitude. The correct isosurface maps are reported here for the collective threshold 0.031 a.u., which was determined via some preliminary tests. This value overrides the 0.5 a.u. value in the published article. Although the shapes of the isosurfaces are somewhat different from those in the published article, the general conclusions arrived at previously regarding the reliability of the anisotropy of the vorticity tensor as a criterion of magnetotropicity are confirmed. In particular, the revised maps show the absence of unequal vorticity in the regions of C–H bonds in planar conjugated hydrocarbons, as well as B–H and N–H bonds in borazine. A domain of enhanced anisotropy of the vorticity tensor is observed in Fig. 6 about the centre of the cyclopropane molecule, whereas the hollow regions appearing in the isosurface, in the proximity of the midpoint of C–C bonds, confirm the absence of σ-diatropicity.
image file: d0cp90097d-f1.tif
Fig. 1 Isosurface with value 0.031 a.u. of the anisotropy of the vorticity tensor in benzene. From the CODATA compilation,2 the conversion factor to SI units is eEh/(a3ħ) = 4.469839112 × 1026 A m−3.

image file: d0cp90097d-f2.tif
Fig. 2 Isosurface with value 0.031 a.u. of the anisotropy of the vorticity tensor in cycloheptatriene cation.

image file: d0cp90097d-f3.tif
Fig. 3 Isosurface with value 0.031 a.u. of the anisotropy of the vorticity tensor in cyclohexane.

image file: d0cp90097d-f4.tif
Fig. 4 Isosurface with value 0.031 a.u. of the anisotropy of the vorticity tensor in cyclohexene.

image file: d0cp90097d-f5.tif
Fig. 5 Isosurface with value 0.031 a.u. of the anisotropy of the vorticity tensor in 1,3-cyclohexadiene.

image file: d0cp90097d-f6.tif
Fig. 6 Isosurface with value 0.031 a.u. of the anisotropy of the vorticity tensor in cyclopropane.

image file: d0cp90097d-f7.tif
Fig. 7 Isosurface with value 0.031 a.u. of the anisotropy of the vorticity tensor in borazine.

image file: d0cp90097d-f8.tif
Fig. 8 Isosurface with value 0.031 a.u. of the anisotropy of the vorticity tensor in cyclobutadiene.

image file: d0cp90097d-f9.tif
Fig. 9 Isosurface with value 0.031 a.u. of the anisotropy of the vorticity tensor in cyclo-octatetraene.

The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers.

Acknowledgements

The authors would like to thank Prof. R. Zanasi for detecting an error in the computer code.

References

  1. R. Zanasi, private communication.
  2. P. J. Mohr, D. B. Newell and B. N. Taylor, Rev. Mod. Phys., 2016, 88, 035009 CrossRef.

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