2019
DOI: 10.1103/physrevb.100.245419
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Induced pairing of fermionic impurities in a one-dimensional strongly correlated Bose gas

Abstract: We investigate numerically the problem of few (one, two) noninteracting spin−1/2 fermions in a shallow harmonic trap coupled via contact repulsive interactions to a uniform one-dimensional bath of lattice bosons, described by the Bose-Hubbard model. Through extensive density-matrix renormalization group calculations, we extract the binding energy and the effective mass of quasiparticles, including dressed impurities (polarons) and their two-body bound states (bipolarons), emerging from the effective non-local … Show more

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Cited by 25 publications
(28 citation statements)
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“…We point out that our results indicate that there is universal dependence of the low temperature T 4 friction force on the impurity velocity in one-dimensional systems as shown by Eqs. (9,26,32,45). This statement is in agreement with the findings of Ref.…”
Section: Conclusion and Discussionsupporting
confidence: 94%
“…We point out that our results indicate that there is universal dependence of the low temperature T 4 friction force on the impurity velocity in one-dimensional systems as shown by Eqs. (9,26,32,45). This statement is in agreement with the findings of Ref.…”
Section: Conclusion and Discussionsupporting
confidence: 94%
“…One possible way to do this is to consider a Bose gas with two mobile impurities, see, e.g., Refs. [20,25,48,49]. We choose another approach.…”
Section: A Bose Gas With Two Impurity Atomsmentioning
confidence: 99%
“…This problem is of current theoretical interest, see Refs. [2,[11][12][13][14][15][16][17][18][19][20][21][22][23][24][25], which provide us with data for benchmarking and interpreting some of our IM-SRG results.…”
Section: Introductionmentioning
confidence: 99%
“…In 1D, the character of this interaction crucially depends on a sign of the boson-impurity coupling constant [35]; the effective attraction is found for positive couplings, while the induced repulsive potential is inherent for the negative interactions. While it increases, the induced attractive interaction between impurities leads to the formation of bipolarons [36] in the continuum and on the lattice [37] and even to the emergence of the two-polaron bound states [38]. In one-dimensional geometries with harmonic trapping, the induced interaction causes the clustering [39] of two initially non-interacting atoms and modifies their quench dynamics [40].…”
Section: Introductionmentioning
confidence: 99%