Carbon nanotubes in almost homogeneous transverse magnetic field: exactly solvable model
arXiv:1306.2115 · doi:10.1088/1751-8113/47/11/115307
Abstract
A class of exactly solvable models describing carbon nanotubes in the presence of an external inhomogeneous magnetic field is considered. The framework of the continuum approximation is employed, where the motion of the charge carriers is governed by the Dirac- Weyl equation. The explicit solution of a particular example is provided. It is shown that these models possess nontrivial integrals of motion that establish N = 2 nonlinear supersymmetry in case of metallic and maximally semiconducting nanotubes. Remarkable stability of energy levels with respect to small fluctuations of longitudinal momentum is demonstrated
17 pages, 6 figures, misprints corrected, references added
References in corpus (8)
- Self-isospectrality, special supersymmetry, and their effect on the band structure
- Hidden supersymmetry in quantum bosonic systems
- Supersymmetry in carbon nanotubes in a transverse magnetic field
- Hidden nonlinear supersymmetry of finite-gap Lame equation
- Supersymmetric twisting of carbon nanotubes
- Exactly solvable associated Lame potentials and supersymmetric transformations
- New supersymmetric partners for the associated Lame potentials
- Finite-gap twists of carbon nanotubes and an emergent hidden supersymmetry
Cited by in corpus (8)
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- Zero Energy States for a Class of Two-Dimensional Potentials in Graphene
- Pseudo-Hermitian Dirac operator on the torus for massless fermions under the action of external fields
- The solutions of Dirac equation on the hyperboloid under perpendicular magnetic fields
- Solvable Two-dimensional Dirac Equation with Matrix Potential: Graphene in External Electromagnetic Field