Two spatially separate neutral atoms can be deterministically entangled in their real-space positions at ~100-micron separation via state-dependent Rydberg blockade and photon recoil.
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Local Boolean kinetic constraints added to Dicke superradiance generate extensive mixed-state entanglement and a hierarchy of long-range entangled singlet dark states while retaining superradiant N^2 scaling.
Variable detuning in Rydberg arrays induces strong Hilbert-space fragmentation whose fragment dimensions exhibit multiple scaling behaviors, with emergent kinetic constraints captured by an auxiliary fermion description.
Quench dynamics in three-level dipole-interacting Rydberg arrays produce scalable spin-nematic squeezing with ξ² ∝ N^{-2/3} (all-to-all symmetric) or N^{-0.7} (antisymmetric), yielding F_Q ∝ N².
Long-range dipolar XY antiferromagnets on a breathed Kagome lattice host a robust chiral spin liquid, with DMRG phase diagrams and AMO-ready preparation and edge probes.
Ytterbium Rydberg pairs naturally realize strongly anisotropic XXZ spin interactions that can be tuned by a magnetic field.
Long-range interactions in the spin-one Heisenberg chain with anisotropy stabilize continuous symmetry breaking phases with logarithmic corrections to entanglement entropy and continuously varying critical exponents.
A scheme is developed to engineer strong three-body interactions in Rydberg atom lattices, allowing the effective Hamiltonian and emergent quantum phases to be modified compared to two-body-only systems.
A 256-qubit Rydberg simulator quantitatively reproduces the magnetization curves and antiferromagnetic transition of TmMgGaO4 while revealing thermalization after quenches.
Sign changes of the new Krylov staggering parameter mark the boundary between edge-localized and bulk-dominated low-energy regimes in the Kitaev chain.
Quantum quenches in the Ising chain exhibit qualitatively distinct out-of-equilibrium dynamics when crossing continuous versus first-order quantum transitions depending on the transverse field strength.
Light-induced losses dominate DyK Feshbach molecule decay in most near-IR traps, but near 2000 nm collisional losses appear and are suppressed by an order of magnitude for the most weakly bound dimers due to Pauli exclusion.
Tuning a femtosecond laser across the two-photon ionization threshold controls the formation of dense Rydberg gas or ultracold plasma in a Rb BEC, with charge imbalance driving the decay as confirmed by electron measurements and simulations.
In Markovian open quantum systems with bistability, noise-induced stochastic switching limits relaxation and follows an Arrhenius law with inverse system size as effective temperature, distinct from deterministic slow relaxation due to a small Liouvillian gap.
citing papers explorer
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Macroscopic position-position entanglement by photon recoil in Rydberg atoms
Two spatially separate neutral atoms can be deterministically entangled in their real-space positions at ~100-micron separation via state-dependent Rydberg blockade and photon recoil.
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Extensive mixed-state entanglement in kinetically constrained superradiance
Local Boolean kinetic constraints added to Dicke superradiance generate extensive mixed-state entanglement and a hierarchy of long-range entangled singlet dark states while retaining superradiant N^2 scaling.
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Emergent Kinetic Constraints and Subspace Fragmentation in Rydberg Arrays
Variable detuning in Rydberg arrays induces strong Hilbert-space fragmentation whose fragment dimensions exhibit multiple scaling behaviors, with emergent kinetic constraints captured by an auxiliary fermion description.
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Scalable spin-nematic squeezing in multi-level dipole-interacting Rydberg atom arrays
Quench dynamics in three-level dipole-interacting Rydberg arrays produce scalable spin-nematic squeezing with ξ² ∝ N^{-2/3} (all-to-all symmetric) or N^{-0.7} (antisymmetric), yielding F_Q ∝ N².
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A Dipolar Chiral Spin Liquid on the Breathed Kagome Lattice
Long-range dipolar XY antiferromagnets on a breathed Kagome lattice host a robust chiral spin liquid, with DMRG phase diagrams and AMO-ready preparation and edge probes.
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Magnetic-field control of interactions in alkaline-earth Rydberg atoms and applications to {\it XXZ} models
Ytterbium Rydberg pairs naturally realize strongly anisotropic XXZ spin interactions that can be tuned by a magnetic field.
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Unconventional entanglement scaling and quantum criticality in the long-range spin-one Heisenberg chain with single-ion anisotropy
Long-range interactions in the spin-one Heisenberg chain with anisotropy stabilize continuous symmetry breaking phases with logarithmic corrections to entanglement entropy and continuously varying critical exponents.
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Three-body interactions in Rydberg lattices
A scheme is developed to engineer strong three-body interactions in Rydberg atom lattices, allowing the effective Hamiltonian and emergent quantum phases to be modified compared to two-body-only systems.
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One-to-one quantum simulation of a frustrated magnet with 256 qubits
A 256-qubit Rydberg simulator quantitatively reproduces the magnetization curves and antiferromagnetic transition of TmMgGaO4 while revealing thermalization after quenches.
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Long-Range Pairing in the Kitaev Model: Krylov Subspace Signatures
Sign changes of the new Krylov staggering parameter mark the boundary between edge-localized and bulk-dominated low-energy regimes in the Kitaev chain.
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Quantum quenches across continuous and first-order quantum transitions in one-dimensional quantum Ising models
Quantum quenches in the Ising chain exhibit qualitatively distinct out-of-equilibrium dynamics when crossing continuous versus first-order quantum transitions depending on the transverse field strength.
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Optically trapped Feshbach molecules of fermionic $^{161}$Dy and $^{40}$K: Role of light-induced and collisional losses
Light-induced losses dominate DyK Feshbach molecule decay in most near-IR traps, but near 2000 nm collisional losses appear and are suppressed by an order of magnitude for the most weakly bound dimers due to Pauli exclusion.
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Ultrafast many-body dynamics of dense Rydberg gases and ultracold plasma
Tuning a femtosecond laser across the two-photon ionization threshold controls the formation of dense Rydberg gas or ultracold plasma in a Rb BEC, with charge imbalance driving the decay as confirmed by electron measurements and simulations.
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Switching Dynamics of Metastable Open Quantum Systems
In Markovian open quantum systems with bistability, noise-induced stochastic switching limits relaxation and follows an Arrhenius law with inverse system size as effective temperature, distinct from deterministic slow relaxation due to a small Liouvillian gap.