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Halo nuclei in a three-body model and universal characteristics of low-energy few-body systems
(2010-12-14)
Within general characteristics of low-energy few-body systems, we revise some well-known correlations found in nuclear physics, and the properties of low-mass halo nuclei in a three-body neutron-neutron-core model. In this ...
Halo nuclei in a three-body model and universal characteristics of low-energy few-body systems
(2010-12-14)
Within general characteristics of low-energy few-body systems, we revise some well-known correlations found in nuclear physics, and the properties of low-mass halo nuclei in a three-body neutron-neutron-core model. In this ...
Three-boson recombination at ultralow temperatures
(Elsevier B.V., 2007-04-09)
The effects of trimer continuum resonances are considered in the three-body recombination rate of a Bose system at finite energies for large and negative two-body scattering lengths (a). The thermal average of the rate ...
Supercircle description of universal three-body states in two dimensions
(Amer Physical Soc, 2012-02-02)
Bound states of asymmetric three-body systems confined to two dimensions are currently unknown. In the universal regime, two energy ratios and two mass ratios provide complete knowledge of the three-body energy measured ...
Supercircle description of universal three-body states in two dimensions
(2012-02-02)
Bound states of asymmetric three-body systems confined to two dimensions are currently unknown. In the universal regime, two energy ratios and two mass ratios provide complete knowledge of the three-body energy measured ...
Quantum propagator for some classes of three-dimensional three-body systems
(2006-05-01)
In this work we solve exactly a class of three-body propagators for the most general quadratic interactions in the coordinates, for arbitrary masses and couplings. This is done both for the constant as the time-dependent ...
Quantum propagator for some classes of three-dimensional three-body systems
(2006-05-01)
In this work we solve exactly a class of three-body propagators for the most general quadratic interactions in the coordinates, for arbitrary masses and couplings. This is done both for the constant as the time-dependent ...