Pantheon SEMPARIS Le serveur des séminaires parisiens Paris

Status Confirmed
Seminar Series SEM-LKB
Subjects quant-ph
Date Wednesday 10 June 2020
Time 14:00
Institute LKB
Seminar Room Visioconférence Zoom
Speaker's Last Name Pfau
Speaker's First Name Tilman
Speaker's Email Address
Speaker's Institution University of Stuttgart
Title Quantum Droplets and Supersolidity in a Dipolar Quantum Gas
Abstract Dipolar interactions are fundamentally different from the usual van der Waals forces in real gases. Besides the anisotropy the dipolar interaction is nonlocal and as such allows for self organized structure formation. In 2005 the first dipolar effects in a quantum gas were observed in an ultracold Chromium gas. By the use of a Feshbach resonance a purely dipolar quantum gas was observed three years after [1]. Recently it became possible to study degenerate gases of lanthanide atoms among which one finds the most magnetic atoms. Similar to the Rosensweig instability in classical magnetic ferrofluids self-organized structure formation was expected. In our experiments with quantum gases of Dysprosium atoms we could observe the formation of a droplet crystal [2]. In contrast to theoretical mean field based predictions the super-fluid droplets did not collapse. We find that this unexpected stability is due to beyond mean-field quantum corrections of the Lee-Huang-Yang type [3,4]. We observe and study self-bound droplets [5] which can interfere with each other. We also observe self-organized stripes in a confined geometry [6] and collective scissors mode oscillations of dipolar droplets [7Recently in the striped phase also phase coherence was observed in Dysprosium and Erbium experiments, which is evidence for a supersolid state of matter [8]. Upon crossing the transition to the dipolar supersolid a Goldstone mode appears, which we have observed recently [9]. The existence of this mode proofs the superfluid stiffness or the so-called phase rigidity of this new state of matter. Despite the lack of symmetry protection, also a Higgs mode was predicted to be observable in a finite system [10]. References [1] T. Lahaye, et al., Rep. Prog. Phys. 72, 126401 (2009) [2] H. Kadau, et al., Nature 530, 194 (2016) [3] T.D. Lee, K. Huang, and C. N. Yang, Phys. Rev. 106, 1135 (1957), D.S. Petrov, Phys. Rev. Lett. 115, 155302 (2015). [4] I. Ferrier-Barbut, et al., Phys. Rev. Lett. 116, 215301 (2016) [5] M. Schmitt, et al., Nature 539, 259 (2016) [6] M. Wenzel, et al., Phys. Rev. A 96 053630 (2017) [7] I. Ferrier-Barbut, et al., Phys. Rev. Lett. 120, 160402 (2018) [8] F. Böttcher, et al. Phys. Rev. X. 9, 011051 (2019), see also L. Tanzi, et al. Phys. Rev. Lett. 122, 130405 (2019), L. Chomaz et al., Phys. Rev. X 9, 021012 (2019) [9] M. Guo, et al. Nature. 574, 386--389 (2019) [10] J. Hertkorn et al., Phys. Rev. Lett. 123, 193002 (2019)
arXiv Preprint Number
Comments Lien zoom : https://us02web.zoom.us/j/81651124927? pwd=Z3pTNlNWeENMclJOeFgzM21DK2xCUT09
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