2018
DOI: 10.1088/1367-2630/aaf295
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Roton in a few-body dipolar system

Abstract: We solve numerically exactly the many-body 1D model of bosons interacting via short-range and dipolar forces and moving in the box with periodic boundary conditions. We show that the lowest energy states with fixed total momentum can be smoothly transformed from the typical states of collective character to states resembling single particle excitations. In particular, we identify the celebrated roton state. The smooth transition is realized by simultaneous tuning short-range interactions and adjusting a trap g… Show more

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Cited by 4 publications
(6 citation statements)
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References 86 publications
(150 reference statements)
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“…Our subject of interest are the lowest energy eigenstatetes with a given total momentum, so called yrast states [21,22]. Here we will consider only the contact interaction for which the yrast states coincide with the type II solitonic elementary excitations (as shown in [23] it does not need to be the case for dipolar interactions).…”
Section: Weakly-interacting Gasmentioning
confidence: 99%
“…Our subject of interest are the lowest energy eigenstatetes with a given total momentum, so called yrast states [21,22]. Here we will consider only the contact interaction for which the yrast states coincide with the type II solitonic elementary excitations (as shown in [23] it does not need to be the case for dipolar interactions).…”
Section: Weakly-interacting Gasmentioning
confidence: 99%
“…We select the interaction parameters so that the histograms have a similar width for attractive and repulsive scenarios. Both histograms are obtained by drawing particles' positions from the many-body probability distribution with the Metropolis algorithm and aligned by rotating them such that their center of mass point in the same direction [26]. We observe two spatially localized boundstates with completely different properties.…”
mentioning
confidence: 96%
“…In the longitudinal directionx the space is assumed to be finite, with the length L. All atoms are polarized along thex axis in head-to-tail configuration [27]. Our quasi-1D system is governed by the Hamiltonian: [26]. Note that for very small systems the peak density value is biased by our alignment method.…”
mentioning
confidence: 99%
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“…The MF regime defined in such a way is very difficult to handle in the frame of many-body analysis, which is usually limited to systems with small number of atoms N. Apart from the few existing semianalytical results [22,24,25], the majority of approaches are devoted to small systems of ≈10-20 atoms [20,21,[33][34][35][36] solved with brute force methods or around ≈100 atoms solved with sophisticated and time-consuming numerics [28,29,37,38]. Our way around these numerical difficulties is to use a natural and simple ansatz for the yrast states in the MF regime.…”
Section: The Lieb-liniger Model and Yrast Statesmentioning
confidence: 99%