2011
DOI: 10.1103/physrevlett.107.246403
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Few-Particle Green’s Functions for Strongly Correlated Systems on Infinite Lattices

Abstract: We show how few-particle Green's functions can be calculated efficiently for models with nearestneighbor hopping, for infinite lattices in any dimension. As an example, for one dimensional spinless fermions with both nearest-neighbor and second nearest-neighbor interactions, we investigate the ground states for up to 5 fermions. This allows us not only to find the stability region of various bound complexes, but also to infer the phase diagram at small but finite concentrations.PACS numbers: 71.10. Li, 31.15.a… Show more

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Cited by 24 publications
(27 citation statements)
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“…We find that for all the detunings ν in figure 1 that cover the SM and FPP phases, the corresponding U in H sc is so negative that the ground state is a droplet with all fermions packed together in a region of the size of N f sites, see figure 10(b). Such cluster bound state was also shown previously for few particles [37]. It can be understood by mapping H sc into a quantum spin chain using the Jordan-Wigner transformation, where the occupied (empty) site is mapped to spin-up (spin-down), and the U(<0) term in equation (12) can be mapped to the ferromagnetic Ising interaction.…”
Section: = åsupporting
confidence: 64%
“…We find that for all the detunings ν in figure 1 that cover the SM and FPP phases, the corresponding U in H sc is so negative that the ground state is a droplet with all fermions packed together in a region of the size of N f sites, see figure 10(b). Such cluster bound state was also shown previously for few particles [37]. It can be understood by mapping H sc into a quantum spin chain using the Jordan-Wigner transformation, where the occupied (empty) site is mapped to spin-up (spin-down), and the U(<0) term in equation (12) can be mapped to the ferromagnetic Ising interaction.…”
Section: = åsupporting
confidence: 64%
“…In this case, the low-energy Hilbert subspace factorizes into two sectors, with the particles being separated either by an even or by an odd number of sites; the remaining terms in the Hamiltonian do not mix these subspaces. To solve for bound states, we calculate the two-particle propagator [38] and check for discrete poles appearing below the continuum. We find thatÛ 0,2 and U 1 can lead to the appearance of a bound state in their respective subspace.…”
mentioning
confidence: 99%
“…To understand the implications of this result, note that the bare particles (λ = 0) bind only for U ≤ −2t. This attraction is needed to compensate for the loss of kinetic energy [69]. The SSH polaron dispersionand hence its kinetic energy -remains significant at all particle -phonon couplings.…”
mentioning
confidence: 99%