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Scalar Charged Particle in Presence of Magnetic and Aharonov-Bohm Fields Plus Scalar-Vector Killingbeck Potentials Sameer M Ikhdair.

Yazar: Materyal türü: MakaleMakaleDil: İngilizce Yayın ayrıntıları:Sprınger Wıen, 2013.ISSN:
  • 0177-7963
Konu(lar): LOC sınıflandırması:
  • QC23
Çevrimiçi kaynaklar: İçindekiler: Few-Body Systems Nov 2013, Vol.54 Issue:11, p.1987-1995Özet: 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 + lambda r (2), 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.
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Online Electronic Document NEU Grand Library Online electronic QC23 .S33 2013 (Rafa gözat(Aşağıda açılır)) Ödünç verilmez EOL-606

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 + lambda r (2), 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.

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