
Two-dimensional supersolidity in a dipolar quantum gas
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ABSTRACT Supersolid states simultaneously feature properties typically associated with a solid and with a superfluid. Like a solid, they possess crystalline order, manifesting as a periodic
modulation of the particle density; but unlike a typical solid, they also have superfluid properties, resulting from coherent particle delocalization across the system. Such states were
initially envisioned in the context of bulk solid helium, as a possible answer to the question of whether a solid could have superfluid properties1,2,3,4,5. Although supersolidity has not
been observed in solid helium (despite much effort)6, ultracold atomic gases provide an alternative approach, recently enabling the observation and study of supersolids with dipolar
atoms7,8,9,10,11,12,13,14,15,16. However, unlike the proposed phenomena in helium, these gaseous systems have so far only shown supersolidity along a single direction. Here we demonstrate
the extension of supersolid properties into two dimensions by preparing a supersolid quantum gas of dysprosium atoms on both sides of a structural phase transition similar to those occurring
in ionic chains17,18,19,20, quantum wires21,22 and theoretically in chains of individual dipolar particles23,24. This opens the possibility of studying rich excitation
properties25,26,27,28, including vortex formation29,30,31, and ground-state phases with varied geometrical structure7,32 in a highly flexible and controllable system. Access through your
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SUPERFLUID FRACTION OF A SUPERSOLID BY JOSEPHSON EFFECT Article Open access 08 May 2024 SUPERSOLIDITY IN ULTRACOLD DIPOLAR GASES Article 09 October 2023 PHASE COHERENCE IN OUT-OF-EQUILIBRIUM
SUPERSOLID STATES OF ULTRACOLD DIPOLAR ATOMS Article 04 January 2021 DATA AVAILABILITY Data pertaining to this work can be found at https://doi.org/10.5281/zenodo.4729519. CODE AVAILABILITY
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041604 (2011). Article ADS CAS Google Scholar Download references ACKNOWLEDGEMENTS We thank the Innsbruck Erbium team, T. Bland, G. Morigi and B. Blakie for discussions. We acknowledge
R. M. W. van Bijnen for developing the code for our eGPE ground-state simulations. The experimental team is financially supported through an ERC Consolidator Grant (RARE, number 681432), an
NFRI grant (MIRARE, number ÖAW0600) of the Austrian Academy of Science, the QuantERA grant MAQS by the Austrian Science Fund FWF number I4391-N. L.S. and F.F. acknowledge the DFG/FWF via FOR
2247/PI2790. M.S. acknowledges support by the Austrian Science Fund FWF within the DK-ALM (number W1259-N27). L.S. thanks the funding by the Deutsche Forschungsgemeinschaft (DFG, German
Research Foundation) under Germany’s Excellence Strategy - EXC-2123 QuantumFrontiers - 390837967. M.A.N. has received funding as an ESQ Postdoctoral Fellow from the European Union’s Horizon
2020 research and innovation programme under the Marie Skłodowska-Curie grant agreement number 801110 and the Austrian Federal Ministry of Education, Science and Research (BMBWF). M.J.M.
acknowledges support through an ESQ Discovery Grant by the Austrian Academy of Sciences. We also acknowledge the Innsbruck Laser Core Facility, financed by the Austrian Federal Ministry of
Science, Research and Economy. Part of the computational results presented have been achieved using the HPC infrastructure LEO of the University of Innsbruck. AUTHOR INFORMATION Author notes
* These authors contributed equally: Matthew A. Norcia, Claudia Politi AUTHORS AND AFFILIATIONS * Institut für Quantenoptik und Quanteninformation, Österreichische Akademie der
Wissenschaften, Innsbruck, Austria Matthew A. Norcia, Claudia Politi, Lauritz Klaus, Maximilian Sohmen, Manfred J. Mark & Francesca Ferlaino * Institut für Experimentalphysik,
Universität Innsbruck, Innsbruck, Austria Claudia Politi, Lauritz Klaus, Elena Poli, Maximilian Sohmen, Manfred J. Mark, Russell N. Bisset & Francesca Ferlaino * Institut für
Theoretische Physik, Leibniz, Universität Hannover, Hanover, Germany Luis Santos Authors * Matthew A. Norcia View author publications You can also search for this author inPubMed Google
Scholar * Claudia Politi View author publications You can also search for this author inPubMed Google Scholar * Lauritz Klaus View author publications You can also search for this author
inPubMed Google Scholar * Elena Poli View author publications You can also search for this author inPubMed Google Scholar * Maximilian Sohmen View author publications You can also search for
this author inPubMed Google Scholar * Manfred J. Mark View author publications You can also search for this author inPubMed Google Scholar * Russell N. Bisset View author publications You
can also search for this author inPubMed Google Scholar * Luis Santos View author publications You can also search for this author inPubMed Google Scholar * Francesca Ferlaino View author
publications You can also search for this author inPubMed Google Scholar CONTRIBUTIONS M.A.N., C.P., L.K., M.S., M.J.M. and F.F. contributed experimental work. E.P. and R.N.B. performed eGPE
calculations. L.S. contributed variational model. All authors contributed to interpretation of results and preparation of manuscript. CORRESPONDING AUTHOR Correspondence to Francesca
Ferlaino. ETHICS DECLARATIONS COMPETING INTERESTS The authors declare no competing interests. ADDITIONAL INFORMATION PEER REVIEW INFORMATION _Nature_ thanks the anonymous reviewers for their
contribution to the peer review of this work. PUBLISHER’S NOTE Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
EXTENDED DATA FIGURES AND TABLES EXTENDED DATA FIG. 1 FOURIER TRANSFORMS OF IN-TRAP IMAGES. The upper row shows individual in-trap images for different trap aspect ratios, as shown in Fig.
2b. The lower row shows the data for the same parameters in the Fourier domain, with _k_ the associated wavenumber. As the trap aspect ratio is increased, the modulation goes from being
present along a single direction to two, and a clear hexagonal pattern is visible. EXTENDED DATA FIG. 2 SUPERSOLID DROPLET ARRAY WITH MORE THAN TWO ROWS. A, In-trap image of a droplet array
with more than two rows. B, Averaged Fourier transform of 309 images in conditions of A, showing that a regular modulated structure persists in the more extended system. C, Calculated ground
state from the eGPE for trap parameters (_f__x_, _f__y__, f__z_) = (22, 55, 140) Hz, and _N_ = 60,000 atoms in the droplets, representative of the experimental conditions in A, B. D,
Averaged TOF interference pattern for the conditions of A, B. The inset shows the measured 2D density profile and the main panel shows a radially averaged density, normalized to the peak
density of the averaged image. The grey lines represent individual trials and the red line is the average. The repeatability of the modulation indicates the presence of phase coherence
between droplets. EXTENDED DATA FIG. 3 PROSPECTS FOR LARGER AND ISOTROPIC DROPLET ARRAYS. The panels show eGPE-calculated ground-state density profiles with fixed average atomic density (see
text) and either fixed atom number and trap volume (upper row) or fixed _f__x_ (lower row). Here _N_ refers to the total number of atoms in the simulation (droplets plus halo), in contrast
to the definition used elsewhere to compare with experimental conditions (droplets only). RIGHTS AND PERMISSIONS Reprints and permissions ABOUT THIS ARTICLE CITE THIS ARTICLE Norcia, M.A.,
Politi, C., Klaus, L. _et al._ Two-dimensional supersolidity in a dipolar quantum gas. _Nature_ 596, 357–361 (2021). https://doi.org/10.1038/s41586-021-03725-7 Download citation * Received:
10 February 2021 * Accepted: 14 June 2021 * Published: 18 August 2021 * Issue Date: 19 August 2021 * DOI: https://doi.org/10.1038/s41586-021-03725-7 SHARE THIS ARTICLE Anyone you share the
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