. 2022 Oct 21;126(43):7864–7873. doi: 10.1021/acs.jpca.2c04856

Table 3. Strength of the Diatropic and Paratropic Contributions (in nA·T^–1) to the Net MICD Strength Passing Different Planes in Molecule 3 and Its Dication^a.

plane	diatropic	paratropic	net
Neutral
3A	6.73	–8.53	–1.79
3B	7.46	–7.74	–0.28
3C	7.61	–7.61	0.00
3D	7.49	–7.49	0.00
3E	6.23	–6.23	0.00
3F	34.96	–14.04	20.92
Dication
3A	22.35	–0.28	22.06
3B	37.11	–0.07	37.04
3C	7.68	–7.68	0.00
3D	7.57	–7.57	0.00
3E	6.28	–6.28	0.00
3F	33.09	–14.73	18.35

The net current strength vanishes for plane 3C due to symmetry, whereas they vanish in planes 3D and 3E because the current-density vortex is localized as shown in Figure 8.

Table 3. Strength of the Diatropic and Paratropic Contributions (in nA·T–1) to the Net MICD Strength Passing Different Planes in Molecule 3 and Its Dicationa.

Table 3. Strength of the Diatropic and Paratropic Contributions (in nA·T^–1) to the Net MICD Strength Passing Different Planes in Molecule 3 and Its Dication^a.