A geometrical interpretation of the Thomas theorem and the Efimov States
arXiv:1811.10412 · doi:10.1088/2399-6528/abaca4
Abstract
Using a generalized Bohr model and the hyper-spherical formalism for a three-body system, we derive the Thomas theorem assuming a simple interaction depending on the range of the potential. We discuss the conditions for which an unbound two-body system produces a bound three-body system and derive universal energy functions. We apply our model to He and Triton atoms as well as to the triton nucleus. Using their scattering lengths and effective ranges, we are able to reproduce the two-body or the three-body binding energies with only one parameter fitted. Prediction for excited (Efimov) levels are also given and in particular we demonstrate that for some hyper-angles two equal minima appear which indicate a phase (shape) transition similar to the Landau's theory of phase transition. We suggest that the observed excited levels in two different experiments for the triton nucleus are indeed Efimov levels and there may be more surprises.
6 pages, 4 figures
References in corpus (10)
- Observation of an Efimov spectrum in an atomic system
- Observation of an Efimov-like resonance in ultracold atom-dimer scattering
- Evidence for Universal Four-Body States Tied to an Efimov Trimer
- Efimov Physics in Cold Atoms
- Nuclear binding near a quantum phase transition
- High precision probe of the fully sequential decay width of the Hoyle state in C
- Linear correlations between 4He trimer and tetramer energies calculated with various realistic 4He potentials
- Modeling B as a B-n-n three-body system in the unitary limit
- Decay Modes of the Hoyle State in
- Strongly Resonating Bosons in Hot Nuclei