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Quantum Information Entropy of Hyperbolic Potentials in Fractional Schrödinger Equation

In this work we have studied the Shannon information entropy for two hyperbolic single-well potentials in the fractional Schrödinger equation (the fractional derivative number [Formula: see text] by calculating position and momentum entropy. We find that the wave function will move towards the origi...

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Detalles Bibliográficos
Autores principales: Santana-Carrillo, R., González-Flores, Jesus S., Magaña-Espinal, Emilio, Quezada, Luis F., Sun, Guo-Hua, Dong, Shi-Hai
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9689018/
https://www.ncbi.nlm.nih.gov/pubmed/36359609
http://dx.doi.org/10.3390/e24111516
Descripción
Sumario:In this work we have studied the Shannon information entropy for two hyperbolic single-well potentials in the fractional Schrödinger equation (the fractional derivative number [Formula: see text] by calculating position and momentum entropy. We find that the wave function will move towards the origin as the fractional derivative number n decreases and the position entropy density becomes more severely localized in more fractional system, i.e., for smaller values of n, but the momentum probability density becomes more delocalized. And then we study the Beckner Bialynicki-Birula–Mycieslki (BBM) inequality and notice that the Shannon entropies still satisfy this inequality for different depth u even though this inequality decreases (or increases) gradually as the depth u of the hyperbolic potential [Formula: see text] (or [Formula: see text]) increases. Finally, we also carry out the Fisher entropy and observe that the Fisher entropy increases as the depth u of the potential wells increases, while the fractional derivative number n decreases.