An array of highly-excited (Rydberg) atoms is an emerging platform for quantum many-bodysimulation and computation. In the talk, I will introduce this modern approach and review its recentsuccesses: e.g. discovery of many-body quantum scars, generation of large entangled states, andimplementation of efficient quantum gates. I believe the topic should be interesting for a broadaudience interested in condensed matter, quantum information, or AMO.
join us at 10:00

Dr. Alexandre Dauphin (ICFO – The Institute of Photonic Sciences, Barcelona)
In the last decades, topological insulators have attracted great interest and also have promising applicationsin topics such as metrology or quantum computation. These exotic materials go beyond the standardclassification of phases of matter: they are insulating in their bulk, conducting on their edges, andcharacterized by a global topological invariant, in contrast to a local order parameter as in the conventionalGinzburg-Landau theory of phases of matter. Such topological phases have been experimentally observed incondensed matter systems and more recently in quantum simulators. The latter are very versatile platformsthat allow one to simulate a material with another quantum system in a very controllable environment. In thecase of topological insulators, this degree of control is particularly promising to unveil the mechanismsleading to these phases. The quantum simulation of these exotic materials typically relies on the generationof artificial gauge fields. However, recent studies have shown that topological phases can also emerge fromparticle interactions. The latter mechanism leads to the concept of interaction-induced topological phases, inwhich topology is acquired through a spontaneous symmetry breaking process. The interplay of thespontaneous symmetry breaking with the global topological properties can lead to very interesting effects.In this talk, I will discuss how such interplay can lead to new strongly-correlated topological effects ina 2D material. In particular, I will show how interactions can localize particles in the insulating bulk atincommensurate fillings, leading to self-trapped polarons. Furthermore at higher filling, the interactingnature of the topological insulator gives rise to domains in the bulk. Interestingly, the nontrivial topologyassociated to each domain leads to the appearance of protected conducting states in the bulk, localized at thedomain boundaries. Finally, I will discuss the possibility of quantum simulating such phases with cold laserexcitedRydberg atoms in an optical lattice.
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mgr Anna Dawid - Łękowska (IFT UW)
Ultracold polar molecules possess a significantly richer internal structure than atoms and offerstrong dipolar interactions due to their permanent electric dipole moment. These two qualities makethem a highly promising platform for quantum simulations. Numerous applications of ultracoldmolecules have been introduced, but particular interest can be noticed in the field of quantummagnetism. Their rotational states (in which pseudo-spins can be encoded) combined with dipolarinteraction and the possibility of control with microwave fields inspired many proposals realizingvarious quantum magnetism models with polar molecules in optical lattices. We follow anotherapproach, focusing on the bound states of two ultracold polar and paramagnetic molecules in aharmonic trap. We show that various magnetization states arise from the interplay of the molecularinteractions, electronic spins, dipole moments, rotational structures, external fields, and spinrotationcoupling. The rich magnetization diagrams depend primarily on the anisotropy of theintermolecular interaction and the spin-rotation coupling. These specific molecular properties arechallenging to calculate or measure. Therefore, we propose the quench dynamics experiments forextracting them from observing the time evolution of the analyzed system. Results provide newinsight into the rich magnetic properties of ultracold molecules and indicate the possibility tocontrol the molecular few-body magnetization with the external electric field. The chosensimplified system is also the first step towards research on the controlled magnetization of manybodymolecular systems in optical tweezers or optical lattices and their application in quantumsimulation of molecular multichannel many-body Hamiltonians and quantum information storing.Instrukcja obsługi połączenia internetowego znajduje się na stronie:https://support.zoom.us/hc/en-us/articles/201362193-Joining-a-Meetinglub w
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Stefan Willitsch (Department of Chemistry, University of Basel)
Inspired by methods established within the realms of quantum optics and atomic-ion quantumtechnologies, we demonstrate a quantum-non-demolition technique for the non-destructivedetection of the internal quantum state of a single trapped molecular ion. The method is based onthe state-dependent coherent excitation of the motion of the trapped molecular ion and subsequentdetection of the motional quantum state using a co-trapped atomic ion. This new approach offersnew perspectives not only for the detection, but also for the preparation and the manipulation ofmolecular quantum states on the single-particle level with a greatly improved sensitivity comparedto previously used destructive schemes. We present a characterization of our technique using thehomonuclear diatomic species N2+ as an example, show how it can be used for non-invasivespectroscopic measurements on single molecules and discuss prospective applications in the realmof precision molecular spectroscopy.
Seminarium z użyciem połączenia internetowegohttps://zoom.us/j/97696726563(meeting ID: ID 97696726563, password: 314297)