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