Analytical study of bound states in graphene nanoribbons and carbon nanotubes: The variable phase method and the relativistic Levinson theorem
Abstract
The problem of localized states in 1D systems with a relativistic spectrum, namely, graphene stripes and carbon nanotubes, is studied analytically. The bound state as a superposition of two chiral states is completely described by their relative phase, which is the foundation of the variable phase method (VPM) developed herein. Based on our VPM, we formulate and prove the relativistic Levinson theorem. The problem of bound states can be reduced to the analysis of closed trajectories of some vector field. Remarkably, the Levinson theorem appears as the Poincaré index theorem for these closed trajectories. The VPM equation is also reduced to the nonrelativistic and semiclassical limits. The limit of a small momentum p{sub y} of transverse quantization is applicable to an arbitrary integrable potential. In this case, a single confined mode is predicted.
 Authors:
 University of New South Wales, School of Physics (Australia)
 Publication Date:
 OSTI Identifier:
 22617242
 Resource Type:
 Journal Article
 Resource Relation:
 Journal Name: Journal of Experimental and Theoretical Physics; Journal Volume: 122; Journal Issue: 6; Other Information: Copyright (c) 2016 Pleiades Publishing, Inc.; Country of input: International Atomic Energy Agency (IAEA)
 Country of Publication:
 United States
 Language:
 English
 Subject:
 71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; 77 NANOSCIENCE AND NANOTECHNOLOGY; BOUND STATE; CARBON NANOTUBES; CHIRALITY; EQUATIONS; GRAPHENE; LEVINSON THEOREM; NANOSTRUCTURES; QUANTIZATION; RELATIVISTIC RANGE; SEMICLASSICAL APPROXIMATION; SPECTRA; VECTOR FIELDS
Citation Formats
Miserev, D. S., Email: d.miserev@student.unsw.edu.au, Email: erazorheader@gmail.com. Analytical study of bound states in graphene nanoribbons and carbon nanotubes: The variable phase method and the relativistic Levinson theorem. United States: N. p., 2016.
Web. doi:10.1134/S1063776116060066.
Miserev, D. S., Email: d.miserev@student.unsw.edu.au, Email: erazorheader@gmail.com. Analytical study of bound states in graphene nanoribbons and carbon nanotubes: The variable phase method and the relativistic Levinson theorem. United States. doi:10.1134/S1063776116060066.
Miserev, D. S., Email: d.miserev@student.unsw.edu.au, Email: erazorheader@gmail.com. 2016.
"Analytical study of bound states in graphene nanoribbons and carbon nanotubes: The variable phase method and the relativistic Levinson theorem". United States.
doi:10.1134/S1063776116060066.
@article{osti_22617242,
title = {Analytical study of bound states in graphene nanoribbons and carbon nanotubes: The variable phase method and the relativistic Levinson theorem},
author = {Miserev, D. S., Email: d.miserev@student.unsw.edu.au, Email: erazorheader@gmail.com},
abstractNote = {The problem of localized states in 1D systems with a relativistic spectrum, namely, graphene stripes and carbon nanotubes, is studied analytically. The bound state as a superposition of two chiral states is completely described by their relative phase, which is the foundation of the variable phase method (VPM) developed herein. Based on our VPM, we formulate and prove the relativistic Levinson theorem. The problem of bound states can be reduced to the analysis of closed trajectories of some vector field. Remarkably, the Levinson theorem appears as the Poincaré index theorem for these closed trajectories. The VPM equation is also reduced to the nonrelativistic and semiclassical limits. The limit of a small momentum p{sub y} of transverse quantization is applicable to an arbitrary integrable potential. In this case, a single confined mode is predicted.},
doi = {10.1134/S1063776116060066},
journal = {Journal of Experimental and Theoretical Physics},
number = 6,
volume = 122,
place = {United States},
year = 2016,
month = 6
}

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