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This article presents a theoretical framework in quantum mechanics that maps nonlinear dual-derivative formalisms onto linear Schrödinger equations featuring position-dependent mass metrics. By analyzing specific potentials like the harmonic oscillator, it demonstrates how deformation parameters effectively alter physical confinement and tunneling probabilities without violating standard linearity principles. The work offers an alternative geometric perspective on existing nonadditive translation approaches within quantum theory.
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Effective Geometry and Position-Dependent Mass in Dual-$q$ Quantum Mechanics

arXiv3 min read

arXiv:2606.12444v1 Announce Type: new Abstract: This work investigates the deformed-derivative formalism introduced by Borges, with emphasis on the relation between the linear operator $D_{(q)}$ and its nonlinear dual counterpart $D^{(q)}$. Directly inserting the dual derivative into the kinetic term leads to a nonlinear Schr\"odinger equation and obscures the usual interpretation of superposition and probability. We show that this nonlinearity can be removed by a simultaneous transformation of the coordinate and of the wave function. The transformed problem is an ordinary linear Schr\"odinger equation in a deformed coordinate, and its representation in the physical coordinate is equivalent to a Hermitian position-dependent-mass (PDM) Hamiltonian. In this formulation, the deformation parameter $q$ determines both the effective mass profile and the associated metric. The formalism is applied to the free particle, the infinite square well, the rectangular barrier, and the harmonic oscillator in the weak-deformation regime. Comparison with the nonadditive-translation approach of Costa Filho \emph{et al.} shows that the Borges dual-$q$ framework provides an alternative route to the same effective geometric structure. For $q1$, the effective length is increased, which lowers the spectrum and suppresses tunneling relative to the undeformed limit $q=1$.

Abstract:This work investigates the deformed-derivative formalism introduced by Borges, with emphasis on the relation between the linear operator $D_{(q)}$ and its nonlinear dual counterpart $D^{(q)}$. Directly inserting the dual derivative into the kinetic term leads to a nonlinear Schrödinger equation and obscures the usual interpretation of superposition and probability. We show that this nonlinearity can be removed by a simultaneous transformation of the coordinate and of the wave function. The transformed problem is an ordinary linear Schrödinger equation in a deformed coordinate, and its representation in the physical coordinate is equivalent to a Hermitian position-dependent-mass (PDM) Hamiltonian. In this formulation, the deformation parameter $q$ determines both the effective mass profile and the associated metric. The formalism is applied to the free particle, the infinite square well, the rectangular barrier, and the harmonic oscillator in the weak-deformation regime. Comparison with the nonadditive-translation approach of Costa Filho \emph{et al.} shows that the Borges dual-$q$ framework provides an alternative route to the same effective geometric structure. For $q<1$, the effective confinement length is reduced, which raises the bound-state spectrum and enhances tunneling; for $q>1$, the effective length is increased, which lowers the spectrum and suppresses tunneling relative to the undeformed limit $q=1$.

arXiv:2606.12444 [quant-ph]

(or arXiv:2606.12444v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2606.12444 Focus to learn more arXiv-issued DOI via DataCite

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Full text under the publisher's open licence · 288 words

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