Few-Body Systems

, Volume 54, Issue 11, pp 1987–1995

Scalar Charged Particle in Presence of Magnetic and Aharonov–Bohm Fields Plus Scalar–Vector Killingbeck Potentials


DOI: 10.1007/s00601-013-0693-2

Cite this article as:
Ikhdair, S.M. Few-Body Syst (2013) 54: 1987. doi:10.1007/s00601-013-0693-2


The generalized form of Killingbeck potential is an attractive Coulomb term plus a linear term and a harmonic oscillator term, i.e. −a/r + br + λr2, which has a useful application in quarkonium spectroscopy. The ground state energy with the corresponding wave function are obtained for any arbitrary m-state in two-dimensional Klein–Gordon equation with equal mixture of scalar–vector Killingbeck potentials in the presence of constant magnetic and singular Ahoronov–Bohm flux fields perpendicular to the plane where the interacting charged particle is confined. The analytical exact iteration method is used in our solution. We obtain the energy eigensolutions for particle and antiparticle corresponding to S(r) = V(r) and S(r) = −V(r) cases, respectively. Some special cases like the Coulomb, harmonic oscillator potentials and the nonrelativistic limits are found in presence and absence of external fields.

Copyright information

© Springer-Verlag Wien 2013

Authors and Affiliations

  1. 1.Department of Electrical and Electronic EngineeringNear East UniversityNorthern Cyprus, NicosiaTurkey
  2. 2.Department of Physics, Faculty of ScienceAn-Najah National UniversityNablusPalestine