KG- oscillators in a spinning cosmic string spacetime and an external magnetic field
Abstract
We study the Klein-Gordon (KG) oscillators in a spinning cosmic string spacetime and an external magnetic field. The corresponding KG-equation is shown to admit a solution in the form of the confluent hypergeometric functions/polynomials. Consequently, the corresponding energies are shown to be given in a quadratic equation of a delicate nature that has to be solved in an orderly manner (for it involves the energies for KG-particles/antiparticles, E=E= E along with the magnetic quantum number m=m = |m|). Following a case-by-case strategy allowed us to clearly observe the effects of the spinning cosmic string on the spectroscopic structure of the KG-oscillators. We have observed that, under some parametric settings, whilst the Landau-like energies of the KG-particles (E=E+), with m=m+, have no explicit dependence on the spinning string parameter or wedge parameter α, the KG-antiparticles (E=E-), with m=m-, have such explicit dependence. Interestingly, the co-existence of a spinning cosmic string and external magnetic field eliminates the effect of the wedge parameter ( a byproduct of the string) for KG-particles (E=E+), with m=m+, but not for the KG-antiparticles (E=E-), with m=m-. Such co-existence is observed to break the symmetry of the energies of the KG-particles and antiparticles about E=0 for KG-oscillators. However, for KG-particles (E=E+), with m=m-, and KG-antiparticles (E=E-), with m=m+, are observed to be unfortunate for being indeterminable. Moreover, for the spinning parameter β >>1, clustering of the energy levels is observed eminent to indicate that there is no distinction between energy levels at such values of β .
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