Table 1 Mean exciton diameters of the zero-momentum states \(| \varvec{0};+,+;0,m \rangle\) and \(| \varvec{0};-,-;0,-m \rangle\) as obtained with the Coulomb and Rytova–Keldysh potentials with \(\varepsilon _{s} = 6\) and \(\varepsilon _{d} = 28\). In the case of the Coulomb potential the radii must be compared to the film thickness, which is \(L_{z} = {6}\,{\hbox {nm}}\).
From: Single-particle properties of topological Wannier excitons in bismuth chalcogenide nanosheets
m | 0 | \(-\,1\) | \(+\,1\) | \(-\,2\) | \(+\,2\) | \(-\,3\) | \(+\,3\) | |
|---|---|---|---|---|---|---|---|---|
\(\sqrt{\langle r^{2}\rangle }\) (nm) | \(V^{\textrm{C}}\) | 2.74 | 4.21 | 5.32 | 6.33 | 7.61 | 9.04 | 9.76 |
\(V^{\textrm{RK}}\) | 5.64 | 7.02 | 7.51 | 8.72 | 9.13 | 10.57 | 10.89 | |