2010
DOI: 10.1103/physreva.81.023612
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Interspecies tunneling in one-dimensional Bose mixtures

Abstract: We study the ground-state properties and quantum dynamics of few-boson mixtures with strong interspecies repulsion in one-dimensional traps. If one species localizes at the center, e.g., due to a very large mass compared to the other component, it represents an effective barrier for the latter, and the system can be mapped onto identical bosons in a double well. For weaker localization, the barrier atoms begin to respond to the light component, leading to an induced attraction between the mobile atoms that may… Show more

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Cited by 30 publications
(45 citation statements)
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“…Other relevant phenomena are the presence of a composite fermionized gas [34][35][36], quantum magnetism [37][38][39], or a crossover between composite fermionization and phase separation [40,41]. Also, these small number bosonic mixtures allow for the study of dynamical phenomena, like the tunneling of one species through the barrier formed by the other species [42,43] or the dynamical emergence of orthogonality catastrophe [44]. This latter, extremely appealing phenomena occurs in a system of two atoms in one species and a third atom in a second species.…”
Section: Introductionmentioning
confidence: 99%
“…Other relevant phenomena are the presence of a composite fermionized gas [34][35][36], quantum magnetism [37][38][39], or a crossover between composite fermionization and phase separation [40,41]. Also, these small number bosonic mixtures allow for the study of dynamical phenomena, like the tunneling of one species through the barrier formed by the other species [42,43] or the dynamical emergence of orthogonality catastrophe [44]. This latter, extremely appealing phenomena occurs in a system of two atoms in one species and a third atom in a second species.…”
Section: Introductionmentioning
confidence: 99%
“…The atoms are transversely confined in the y and z directions with the trap frequencies ω ⊥ . The size of the ground-state wave function in the transverse motion is a ⊥ = √h /m α ω ⊥ [26,27], where m e and m g are nearly equal. Since the transverse frequencies are much larger than the trap frequency in the x direction, the transverse motions of the atoms are frozen out.…”
Section: A Two-component Condensate Trapped In a Double-well Potentialmentioning
confidence: 99%
“…(27) in the limit of strong tunnel coupling. We express the Hamiltonian in term of the symmetric-mode and asymmetric-mode operators as H =h( − J e )e † + e + +h( + J e )e † − e − −hJ…”
Section: Appendix : Validity Of the Effective Hamiltonian In The Stromentioning
confidence: 99%
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