Spherical topological-insulator nanoparticles: Quantum size effects and optical transitions
arXiv:1906.08162 · doi:10.1103/PhysRevB.100.205417
Abstract
We have investigated the interplay between band inversion and size quantization in spherically shaped nanoparticles made from topological-insulator (TI) materials. A general theoretical framework is developed based on a versatile continuum-model description of the TI bulk band structure and the assumption of a hard-wall mass confinement. Analytical results are obtained for the wave functions of single-electron energy eigenstates and the matrix elements for optical transitions between them. As expected from spherical symmetry, quantized levels in TI nanoparticles can be labeled by quantum numbers and for total angular momentum and its projection on an arbitrary axis. The fact that TIs are narrow-gap materials, where the charge-carrier dynamics is described by a type of two-flavor Dirac model, requires to assume half-integer values and also causes a doubling of energy-level degeneracy where two different classes of states are distinguished by being parity eigenstates with eigenvalues . The existence of energy eigenstates having the same but opposite parity enables optical transitions where is conserved, in addition to those adhering to the familiar selection rule where changes by . All optical transitions satisfy the usual selection rule . We treat intra- and inter-band optical transitions on the same footing and establish ways for observing unusual quantum-size effects in TI nanoparticles, including oscillatory dependences of the band gap and of transition amplitudes on the nanoparticle radius. Our theory also provides a unified perspective on multi-band models for charge carriers in semiconductors and Dirac fermions from elementary-particle physics.
arXiv comment13 pages, 4 figures, RevTex4.2, v2: extended discussion of optical transitions, including new Figs. 3 & 4, to appear in PRB
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