Cargando…

Classical harmonic three-body system: an experimental electronic realization

The classical three-body harmonic system in [Formula: see text] ([Formula: see text] ) with finite rest lengths and zero total angular momentum [Formula: see text] is considered. This model describes the dynamics of the [Formula: see text] near-equilibrium configurations of three point masses [Formu...

Descripción completa

Detalles Bibliográficos
Autores principales: Escobar-Ruiz, A. M., Quiroz-Juarez, M. A., Del Rio-Correa, J. L., Aquino, N.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9349263/
https://www.ncbi.nlm.nih.gov/pubmed/35922544
http://dx.doi.org/10.1038/s41598-022-17541-0
Descripción
Sumario:The classical three-body harmonic system in [Formula: see text] ([Formula: see text] ) with finite rest lengths and zero total angular momentum [Formula: see text] is considered. This model describes the dynamics of the [Formula: see text] near-equilibrium configurations of three point masses [Formula: see text] with arbitrary pairwise potential [Formula: see text] that solely depends on the relative distances between bodies. It exhibits an interesting mixed regular and chaotic dynamics as a function of the energy and the system parameters. The corresponding harmonic quantum system plays a fundamental role in atomic and molecular physics. In this work we report on a novel electronic experimental realization of the model as a complementary tool to analyze the rich dynamics of the classical system. Our setup allows us to experimentally explore different regions of behavior due to the fact that the intrinsic parameters and initial states of the system are independently set by voltage inputs. Chaotic and periodic motions are characterized employing time series, phase planes, and the largest Lyapunov exponents as a function of the energy and system parameters. The results show an excellent qualitative as well as quantitative agreement between theory and experiment.