Confined Klein-Gordon oscillators in Minkowski spacetime and a pseudo-Minkowski spacetime with a space-like dislocation: PDM KG-oscillators, isospectrality and invariance

TL;DR

This paper investigates the effects of space-like dislocation on Klein-Gordon oscillators in Minkowski and pseudo-Minkowski spacetimes, exploring energy shifts, isospectrality, invariance, and introducing position-dependent mass settings with various confinement potentials.

Contribution

It introduces a new analysis of Klein-Gordon oscillators with space-like dislocation, including isospectrality in pseudo-Minkowski spacetime and various position-dependent mass models with different confinement potentials.

Findings

Energy levels shift due to dislocation, causing unavoidable crossings.

Existence of isospectral and invariant KG-particles in pseudo-Minkowski spacetime.

Illustrative examples of PDM KG-oscillators with different scalar multipliers.

Abstract

We revisit the a confined (in a Cornell-type Lorentz scalar potential) KG-oscillator in Minkowski spacetime with space-like dislocation background. We show that the effect of space-like dislocation is to shift the energy levels along the dislocation parameter axis, and consequently energy levels crossings are unavoidable. We report some KG-particles in a pseudo-Minkowski spacetime with space-like dislocation that admit isospectrality and invariance with the confined KG-oscillator in Minkowski spacetime with space-like dislocation. An alternative PDM setting for the KG-particles (relativistic particles in general) is introduced. We discuss the effects of space-like dislocation and PDM settings on the confined KG-oscillators in Minkowski spacetime with space-like dislocation. Three confined PDM KG-oscillators are discussed as illustrative examples, (i) a PDM KG-oscillator from a dimensionless scalar multiplier $g\left( r\right) =\, exp(2\alpha r^2)\geq0,\, \alpha\,\geq 0$, (ii) a PDM KG-oscillator from a power law type dimensionless scalar multiplier $g\left( r\right) =Ar^{\sigma }\geq0$, and (iii) a PDM KG-oscillator in a Cornnell-type confinement with a dimensionless scalar multiplier $g\left( r\right) =\exp \left( \xi r\right)\geq0$