Infinite bound states and $1/n$ energy spectrum induced by a
Coulomb-like potential of type III in a flat band system
- URL: http://arxiv.org/abs/2205.10477v1
- Date: Sat, 21 May 2022 01:09:04 GMT
- Title: Infinite bound states and $1/n$ energy spectrum induced by a
Coulomb-like potential of type III in a flat band system
- Authors: Yi-Cai Zhang
- Abstract summary: We investigate the bound states in a one-dimensional spin-1 flat band system with a Coulomb-like potential of type III.
Near the threshold of continuous spectrum, the bound state energy is consistent with the ordinary hydrogen-like atom energy level formula.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: In this work, we investigate the bound states in a one-dimensional spin-1
flat band system with a Coulomb-like potential of type III, which has a unique
non-vanishing matrix element in basis $|1\rangle$. It is found that, for such a
kind of potential, there exists infinite bound states. Near the threshold of
continuous spectrum, the bound state energy is consistent with the ordinary
hydrogen-like atom energy level formula with Rydberg correction. In addition,
the flat band has significant effects on the bound states. For example, there
are infinite bound states which are generated from the flat band. Furthermore,
when the potential is weak, the bound state energy is proportional to the
Coulomb-like potential strength $\alpha$. When the bound state energies are
very near the flat band, they are inversely proportional to the natural number
$n$ (e.g., $E_n\propto 1/n, n=1,2,3,...$). Further we find that the energy
spectrum can be well described by quasi-classical approximation (WKB method).
Finally, we give a critical potential strength $\alpha_c$ at which the bound
state energy reaches the threshold of continuous spectrum. \textbf{After
crossing the threshold, the bound states in the continuum (BIC) may exist in
such a flat band system.
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