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Quantum crystals in a trapped Rydberg-dressed Bose-Einstein condensate

Quantum Gases · Submitted 26 Sep 2011

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim As a result described by a mean-field order parameter, such states simultaneously possess crystalline and superfluid properties.

how it is stated · asserted 1.00 read the record →

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arXiv ID1109.5480 (version 2)
Pith IDQB62JNNQ, Pith's permanent record of this paper and its review
CitationC.-H. Hsueh, T.-C. Lin, T.-L. Horng, W. C. Wu. "Quantum crystals in a trapped Rydberg-dressed Bose-Einstein condensate." arXiv:1109.5480 (2011). https://pith.science/paper/QB62JNNQ
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The compiled record

The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,919 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.09 · human participants 0.01 · controlled comparison 0.04 · randomized assignment 0.01 · states quantitative result 0.09 · compares with prior results 0.08 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

Spontaneously crystalline ground states, called quantum crystals, of a trapped Rydberg-dressed Bose-Einstein condensate are numerically investigated. As a result described by a mean-field order parameter, such states simultaneously possess crystalline and superfluid properties. A hexagonal droplet lattice is observed in a quasi-two-dimensional system when dressing interaction is sufficiently strong. Onset of these states is characterized by a drastic drop of the non-classical rotational inertia proposed by Leggett [Phys. Rev. Lett. 25, 1543 (1970)]. In addition, an AB stacking bilayer lattice can also be attained. Due to an anisotropic interaction possibly induced by an external electric field, transition from a hexagonal to a nearly square droplet lattice is also observed.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 Spontaneously crystalline ground states, called quantum crystals, of a trapped Rydberg-dressed Bose-Einstein condensate are numerically investigated. contribution 0.99 0.91 0.13 asserted 0.97
s1 As a result described by a mean-field order parameter, such states simultaneously possess crystalline and superfluid properties. result 0.67 0.77 0.35 asserted 1.00
s2 A hexagonal droplet lattice is observed in a quasi-two-dimensional system when dressing interaction is sufficiently strong. result 1.00 0.91 0.25 asserted 1.00
s3 Onset of these states is characterized by a drastic drop of the non-classical rotational inertia proposed by Leggett [Phys. Rev. Lett. 25, 1543 (1970)]. result 0.93 0.66 0.13 asserted 1.00
s4 In addition, an AB stacking bilayer lattice can also be attained. result 1.00 0.89 0.08 asserted 0.69
s5 Due to an anisotropic interaction possibly induced by an external electric field, transition from a hexagonal to a nearly square droplet lattice is also observed. result 1.00 0.88 0.09 asserted 0.55

What kind of paper the classifier reports this is: simulation study 1.00 · evidence from simulation or computation 1.00.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

Spontaneously crystalline ground states, called quantum crystals, of a trapped Rydberg-dressed Bose-Einstein condensate are numerically investigated. As a result described by a mean-field order parameter, such states simultaneously possess crystalline and superfluid properties. A hexagonal droplet lattice is observed in a quasi-two-dimensional system when dressing interaction is sufficiently strong. Onset of these states is characterized by a drastic drop of the non-classical rotational inertia proposed by Leggett [Phys. Rev. Lett. 25, 1543 (1970)]. In addition, an AB stacking bilayer lattice can also be attained. Due to an anisotropic interaction possibly induced by an external electric field, transition from a hexagonal to a nearly square droplet lattice is also observed.

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