- Hybrid discrete-continuous truncated Wigner approximation for driven, dissipative spin systems (B2)
- Improving mean-field theory for bosons in optical lattices via degenerate perturbation theory (B5)
- Kapitza Trap for Ultracold Atoms (B3)
- Kondo coherence versus superradiance in THz radiation-driven heavy-fermion systems (B1)
- Kramers Moyal coefficients for stochastic processes (B1)
- Level statistics of the one-dimensional dimerized Hubbard model (B4)
- Level statistics of the one-dimensional ionic Hubbard model (B3, B4)
- Light-Cone and Diffusive Propagation of Correlations in a Many-Body Dissipative System (B3)
- Limits of topological protection under local periodic driving (A5, B6, C1, C4)
- Majorana edge modes in a spinful-particle conserving model (B4)
- Many-body dynamics of holes in a driven, dissipative spin chain of Rydberg superatoms (B2)
- Mapping as a probe for heating suppression in periodically driven quantum many-body systems (A6, B6)
- Mean-field approach to Rydberg facilitation in a gas of atoms at high and low temperatures (B2)
- Measuring Entropy and Short-Range Correlations in the Two-Dimensional Hubbard Model (B4)
- Measuring finite-range phase coherence in an optical lattice using Talbot interferometry (B3)
- Melting of the critical behavior of a Tomonaga-Luttinger liquid under dephasing (B4)
- Microscopic dynamics and an effective Landau-Zener transition in the quasiadiabatic preparation of spatially ordered states of Rydberg excitations (B2)
- Momentum-resolved Floquet-engineered pair and single-particle filter in the Fermi-Hubbard model (A5, B4)
- Nanomechanically-induced nonequilibrium quantum phase transition to a self-organized density wave of a Bose-Einstein condensate (A2, B6)
- Non-equilibrium evolution of Bose-Einstein condensate deformation in temporally controlled weak disorder (B5, B6)
