2014
DOI: 10.1103/physreva.90.033601
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Ground-state properties of ultracold trapped bosons with an immersed ionic impurity

Abstract: We consider a trapped atomic ensemble of interacting bosons in the presence of a single trapped ion in a quasi-one-dimensional geometry. Our study is carried out by means of the newly developed multilayer-multiconfiguration time-dependent Hartree method for bosons, a numerical exact approach to simulate quantum many-body dynamics. In particular, we are interested in the scenario by which the ion is so strongly trapped that its motion can be effectively neglected. This enables us to focus on the atomic ensemble… Show more

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Cited by 50 publications
(48 citation statements)
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“…In recent years, a significant effort has been undertaken to simulate in a numerically efficient way the many-body Schrödinger equation describing an ion in a one-dimensional atomic cloud. The ground-state properties of ultracold bosons in interaction with a static (i.e., tightly trapped) ion impurity have been investigated by (Schurer et al, 2014) by means of the multiconfigurational time-dependent Hartree method for bosons (Alon et al, 2008;Cao et al, 2013;Krönke et al, 2013). A harmonically trapped ensemble of atoms with a static ion has been considered, with the effective 1D Hamiltonian…”
Section: Quantum Defect Theorymentioning
confidence: 99%
“…In recent years, a significant effort has been undertaken to simulate in a numerically efficient way the many-body Schrödinger equation describing an ion in a one-dimensional atomic cloud. The ground-state properties of ultracold bosons in interaction with a static (i.e., tightly trapped) ion impurity have been investigated by (Schurer et al, 2014) by means of the multiconfigurational time-dependent Hartree method for bosons (Alon et al, 2008;Cao et al, 2013;Krönke et al, 2013). A harmonically trapped ensemble of atoms with a static ion has been considered, with the effective 1D Hamiltonian…”
Section: Quantum Defect Theorymentioning
confidence: 99%
“…The interaction between the ion at z I and an atom at z A behaves in 1D at large distances as e z z (2( ) ) 2 A I 4 α − − up to a minimal cutoff distance R 1D [32], where α is the polarizability of the atoms and e the elementary charge. For numerical many-body simulations with MCTDHB it is more convenient, however, to define a model potential as [28]:…”
Section: Model Of the Systemmentioning
confidence: 99%
“…Their combination defines indeed a new quantum system characterised by an interaction with different energy and length scales with respect to ultracold atoms, which allows to study the formation of molecular ions [13,14], polarons [15], density bubbles [16], mesoscopic entanglement [17,18], novel ground state properties [19] and collective excitations [20], and quantum information processing [21][22][23]. Further, the interaction of the atoms with the phonons of an ion crystal may serve to investigate solid-state phenomena [24].…”
Section: Introductionmentioning
confidence: 99%