Weak interactions in ac-shaken ring lattices allow supercurrent-based atomtronic angular accelerometers to surpass the Fourier-limited sensitivity scaling of non-interacting atoms by over two orders of magnitude.
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Experimental realization of tunable anomalous Floquet topological phases in a 1D optical lattice via multi-frequency control of gap windings and phase-sensitive detection.
A dissipative protocol with nonreciprocal auxiliary atoms stabilizes arbitrary correlated states across the many-body spectrum in Rydberg arrays.
Two-body interactions cause charge pumping to lose quantization in the driven Falicov-Kimball model despite persisting edge modes, due to interaction-induced broadening, with distinct energy dissipation rates in high- versus intermediate-frequency regimes.
citing papers explorer
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Enhancing supercurrent-based inertial sensing via interactions in atomtronic angular accelerometers
Weak interactions in ac-shaken ring lattices allow supercurrent-based atomtronic angular accelerometers to surpass the Fourier-limited sensitivity scaling of non-interacting atoms by over two orders of magnitude.
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Experimental engineering of Floquet topological phases in a one-dimensional optical lattice
Experimental realization of tunable anomalous Floquet topological phases in a 1D optical lattice via multi-frequency control of gap windings and phase-sensitive detection.
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Dissipative Preparation of Correlated Quantum States in Dipolar Rydberg Arrays
A dissipative protocol with nonreciprocal auxiliary atoms stabilizes arbitrary correlated states across the many-body spectrum in Rydberg arrays.
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Effect of Two-Body Interactions on Floquet topological phases
Two-body interactions cause charge pumping to lose quantization in the driven Falicov-Kimball model despite persisting edge modes, due to interaction-induced broadening, with distinct energy dissipation rates in high- versus intermediate-frequency regimes.