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. 2021 Feb 1;60(11):5876–5881. doi: 10.1002/anie.202017124

Figure 1.

Figure 1

Charge distribution on a pyramidal tip for an uncharged Li electrode (left), and electrostatic potential contours (right) when the tip is in contact with a medium obeying the linear Poisson–Boltzmann equation with a Debey length of about 10 Å; the plot shows a cross section along the diagonal of the tip.