Universal description of the rotational-vibrational spectrum of three particles with zero-range interactions
arXiv:0709.4151 · doi:10.1134/S002136400722002X
Abstract
A comprehensive universal description of the rotational-vibrational spectrum for two identical particles of mass and the third particle of the mass in the zero-range limit of the interaction between different particles is given for arbitrary values of the mass ratio and the total angular momentum . If the two-body scattering length is positive, a number of vibrational states is finite for , zero for , and infinite for . If the two-body scattering length is negative, a number of states is either zero for or infinite for . For a finite number of vibrational states, all the binding energies are described by the universal function , where , ,and is the vibrational quantum number. This scaling dependence is in agreement with the numerical calculations for and only slightly deviates from those for . The universal description implies that the critical values and increase as and , respectively, while a number of vibrational states for is within the range .
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- Atom-dimer scattering length for fermions with different masses: analytical study of limiting cases
- Atom-dimer scattering amplitude for fermionic mixtures with different masses: s-wave and p-wave contributions
- Universality of excited three-body bound states in one dimension
- Fermionic trimers in spin-dependent optical lattices
- Minlos-Faddeev regularization of zero-range interactions in the three-body problem
- Effects of Efimov states on quench dynamics in a three-boson trapped system
- Energetics of three interacting mass-imbalanced bodies in a three-dimensional spherical harmonic trap
- The Efimov effect for heteronuclear three-body systems at positive scattering length and finite temperature
- Shallow Trimers of Two Identical Fermions and One Particle in Resonant Regimes
- Mass-ratio condition for non-binding of three two-component particles with contact interactions
- Universal spectrum of isolated three-body resonances