We study the problem of three ultracold fermions in different hyperfine states loaded into a lattice with spatial dimension D = 1,2. We consider SU(3)-symmetric attractive interactions and also eventually include a three-body constraint, which mimics the effect of three-body losses in the strong-loss regime. We combine exact diagonalization with the Lanczos algorithm, and evaluate both the eigenvalues and the eigenstates of the problem. In D = 1, we find that the ground state is always a three-body bound state (trion) for arbitrarily small interaction, while in D = 2, due to the stronger influence of finite-size effects, we are not able to provide conclusive evidence of the existence of a finite threshold for trion formation. Our data are, however, compatible with a threshold value which vanishes logarithmically with the size of the system. Moreover, we are able to identify the presence of a fine structure inside the spectrum, which is associated with off-site trionic states. The characterization of these states shows that only the long-distance behavior of the eigenstate wave functions provides clear-cut signatures about the nature of bound states and that on-site observables are not enough to discriminate between them. The inclusion of a three-body constraint due to losses promotes these off-site trions to the role of lowest-energy states, at least in the strong-coupling regime. DOI: 10.1103/PhysRevA.87.023617

Trion and dimer formation in three-color fermions

Privitera A;
2013

Abstract

We study the problem of three ultracold fermions in different hyperfine states loaded into a lattice with spatial dimension D = 1,2. We consider SU(3)-symmetric attractive interactions and also eventually include a three-body constraint, which mimics the effect of three-body losses in the strong-loss regime. We combine exact diagonalization with the Lanczos algorithm, and evaluate both the eigenvalues and the eigenstates of the problem. In D = 1, we find that the ground state is always a three-body bound state (trion) for arbitrarily small interaction, while in D = 2, due to the stronger influence of finite-size effects, we are not able to provide conclusive evidence of the existence of a finite threshold for trion formation. Our data are, however, compatible with a threshold value which vanishes logarithmically with the size of the system. Moreover, we are able to identify the presence of a fine structure inside the spectrum, which is associated with off-site trionic states. The characterization of these states shows that only the long-distance behavior of the eigenstate wave functions provides clear-cut signatures about the nature of bound states and that on-site observables are not enough to discriminate between them. The inclusion of a three-body constraint due to losses promotes these off-site trions to the role of lowest-energy states, at least in the strong-coupling regime. DOI: 10.1103/PhysRevA.87.023617
2013
Istituto Officina dei Materiali - IOM -
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/282104
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