paper

Tunable Bands in 1D Fractional Quantum Media

arXiv:2511.18574 · doi:10.1103/yrtd-m3tt

Abstract

Fractional calculus has become an essential framework in geophysics, optics, and biological systems to capture long-range correlations and anomalous transport. In this article, we extend this framework to explore a particle in a periodic potential, where the Schrodinger equation is extended to its fractional form. This allows us to study how the Levy index governs the formation and inversion of energy bands, offering a pathway to engineer new physical behaviors by tuning in periodic quantum systems. We solve the fractional Schrodinger equation (FSE) for periodic rectangular potentials of varying height , barrier thickness , and well width using an imaginary-time evolution algorithm, supplemented by Gaussian process regression. This analysis reveals a qualitative shift in the system's band structure at , separating into distinct regimes of dispersion for and . For , the energy bands invert as symmetric minima emerge within the first Brillouin zone and shift from toward with increasing . These degenerate minima define a Bloch-momentum qubit, suggesting an analog to valley degrees of freedom in valleytronics. The at which inversion completes scales as , , and when varying parameters individually, indicating a tunable sensitivity to potential geometry. In contrast, for , the ground band hardens around , with a dispersion following near . This suggests an effective mass of 0 for at the band's lowest energy state. These results demonstrate that the Levy index serves as a tunable degree of freedom in quantum periodic systems, capable of driving band inversion, modulating the band gap, and reshaping carrier dynamics through effective-mass control.

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