Stability of three-fermion clusters with finite range of attraction
arXiv:1308.4220 · doi:10.1209/0295-5075/103/27005
Abstract
Three quantum particles with on-site repulsion and nearest-neighbour attraction on a one-dimensional lattice are considered. The three-body Schroedinger equation is reduced to a set of single-variable integral equations. Energies of three-particle bound complexes (trions) are found from self-consistency of the approximating matrix equation. In the case of spin-1/2 fermions, the ground state trion energy, the excited state energies, the trion spectra and stability regions are obtained for total spins S = 1/2 and S = 3/2. In the S = 1/2 sector, a narrow but finite parameter region is identified where the ground state consists of a stable fermion pair and an unbound fermion. Also presented is the reference case of spin-0 bosons.
6 pages, 5 figures, plus 3 pages of supplementary material
References in corpus (5)
- Three-body bound states in a lattice
- Lattice two-body problem with arbitrary finite range interactions
- Bound states in the one-dimensional two-particle Hubbard model with an impurity
- Few-particle Green's functions for strongly correlated systems on infinite lattices
- Trion and Dimer Formation of Three-Color Fermions
Cited by in corpus (11)
- Ferromagnetism and Borromean binding in three-fermion clusters
- Trion states and quantum criticality of attractive SU(3) Dirac fermions
- Two-particle bound states on a lattice
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- Ubiquitous light real-space pairing from long-range hopping and interactions
- Stable pair liquid phase in fermionic systems
- Kinetic formation of trimers in a spinless fermionic chain
- Fermion pairing in body-centered-cubic quantum simulators of extended Hubbard models
- Trion formation and unconventional superconductivity in a three-dimensional model with short-range attraction
- Slow transport and bound states for spinless fermions with long-range Coulomb interactions on one-dimensional lattices
- Particle pairing causes subdiffusion of heavy particles in the imbalanced Hubbard model