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Bragg scattering of an ultracold dipolar gas across the phase transition from Bose-Einstein condensate to supersolid in the free-particle regime

D. Petter1, A. Patscheider1, G. Natale1, M. J. Mark1,2, M. A. Baranov2,3, R. van Bijnen2,3, S. M. Roccuzzo4,5, A. Recati4,5, B. Blakie6,7 et al.

D. Baillie6,7, L. Chomaz1, and F. Ferlaino1,2,*

  • 1Institut für Experimentalphysik, Universität Innsbruck, Technikerstraße 25, 6020 Innsbruck, Austria
  • 2Institut für Quantenoptik und Quanteninformation, Österreichische Akademie der Wissenschaften, Technikerstraße 21a, 6020 Innsbruck, Austria
  • 3Center for Quantum Physics, University of Innsbruck, 6020 Innsbruck, Austria
  • 4INO-CNR BEC Center and Dipartimento di Fisica, Università degli Studi di Trento, 38123 Povo, Italy
  • 5Trento Institute for Fundamental Physics and Applications, INFN, 38123 Trento, Italy
  • 6The Dodd-Walls Centre for Photonic and Quantum Technologies, University of Otago, Dunedin 9054, New Zealand
  • 7Department of Physics, University of Otago, Dunedin 9016, New Zealand

  • *Author to whom correspondence and requests for materials should be addressed: Francesca.ferlaino@uibk.ac.at

Phys. Rev. A 104, L011302 – Published 22 July, 2021

DOI: https://doi.org/10.1103/PhysRevA.104.L011302

Abstract

We present an experimental and theoretical study of the response of a dipolar supersolid to a Bragg excitation at high-energy defined by the impulse approximation regime. We experimentally observe a continuous reduction of the response when tuning the contact interaction from an ordinary Bose-Einstein condensate to a supersolid state and ultimately to an incoherent array of droplets. Already in the supersolid regime, the observed reduction is faster than the one theoretically predicted by the Bogoliubov–de Gennes theory. By comparing experiments and theories, we are able to attribute this discrepancy to the presence of coherent phase dynamics induced by the crossing of the phase transition. The phase variations are found to change character along the phase diagram and become predominantly incoherent only when reaching the incoherent-droplet regime.

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