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HL: Fachverband Halbleiterphysik

HL 6: Materials and Devices for Quantum Technology I

HL 6.13: Vortrag

Montag, 17. März 2025, 18:15–18:30, H13

Electric-circuit realization of the Floquet-SSH-Model — •Christine Barko2, Alexander Stegmaier1, Alexander Fritzsche1, Riccardo Sorbello1, Martin Greiter1, Hauke Brand2, Maximilian Hofer2, Udo Schwingenschlögl3, Roderich Moessner4,5, Ching Hua Lee6, Alexander Szameit5,7, Andrea Alù8,9, Tobias Kießling2,5, and Ronny Thomale1,51Physikalisches Inst. (TP1), Universität Würzburg, Würzburg, Germany — 2Physikalisches Inst. (EP3), Universität Würzburg, Würzburg, Germany — 3Physical Science and Engineering Division, King Abdullah University of Science and Technology (KAUST), Thuwal, Saudi Arabia — 4Max Planck Institute for the Physics of Complex Systems, Nöthnitzer Straße 38, Dresden, Germany — 5Würzburg-Dresden Cluster of Excellence ct.qmat, Würzburg, Germany — 6Department of Physics, National University of Singapore, Singapore — 7Institute of Physics, University of Rostock, Rostock, Germany — 8Photonics Initiative, Advanced Science Research Center, City University of New York, New York, USA — 9Physics Program, Graduate Center, City University of New York, New York, USA

We build Floquet-driven capactive circuit networks to realize topological states of matter in the frequency domain. We find the Floquet circuit network equations of motion to reveal a potential barrier which effectively acts as a boundary in frequency space. By implementing a Su-Shrieffer-Heeger Floquet lattice model and measuring the associated circuit Laplacian and characteristic resonances, we demonstrate how topological edge modes can nucleate at such a frequency boundary.

Keywords: Topoelectric circuits; Floquet Systems; Floquet Su-Shrieffer-Heeger model

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