Search arXiv⌕ Search

arXiv · 2610.20723

Boundary-induced geometrical frustration in a square Rydberg-atom lattice

Abstract

We study geometric defects in square-lattice Rydberg-atom arrays induced by lattice-size parity in the striated density-wave phase. While odd-sized lattices select a single striated domain, even-sized lattices seed incompatible domains at the four corners, resulting in a π/2-rotation invariant state with a geometrical defect emanating from the lattice center. At larger detunings, we instead identify a π-rotation-invariant state with two domains nucleated by opposite corners and separated by a one-dimensional diagonal defect. We probe the state-preparation protocol on the Aquila atomic quantum processor and benchmark it with equilibrium and real-time dynamics tensor-network simulations. Our results assess the role of boundaries and lattice size in determining the global ordering in programmable quantum matter.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Marco Rigobello, Luka Pavešić, Daniel Jaschke, Pietro Silvi, Marco Di Liberto, Simone Montangero, Simone Notarnicola. 2026-10-20. Boundary-induced geometrical frustration in a square Rydberg-atom lattice. https://arxiv.org/abs/2610.20723

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Geometry-controlled zeros of resonant Kelvin-wave conversion in four spatial dimensions

Kelvin waves carry energy along vortices, but their resonant interactions contain information that is absent from the linear spectrum. We identify a geometry that exposes this information on a vortex surface in four spatial dimensions. Perpendicular incoming waves cancel the complete local-area four-wave coupling, leaving the finite nonlocal interaction mediated by the surrounding fluid. This interaction restores conversion at generic wave-number ratios, yet changes sign and vanishes at a selected ratio while momentum and frequency remain exactly matched. Matching to Gross-Pitaevskii (GP) theory, including the microscopic core response, establishes a zero of the full coupling at every sufficiently small nonzero wave number, with ratio tending to $λ_*\simeq1.469$. Finite-grid GP coefficients exhibit a sign reversal for the same resonant quartets. Separate coherent-mixing calculations and weak-probe spectra connect the coupling sign to the generated-wave phase and the ordering of reflection-even and reflection-odd modes. The resulting suppression removes a leading channel for changing propagation directions without changing the paired wavelengths. These results isolate a nonlinear effect of the surrounding flow that local tension misses, providing a microscopic benchmark for vortex-wave theories and a starting point for studying angular redistribution beyond the Kelvin spectrum.

cond-mat.quant-gas↗

Entropy transport through a superfluid quantum point contact: A Keldysh field-theory approach

We study the matter and entropy transport between two ultra-cold neutral Fermi-gas reservoirs linked by a quantum point contact under a chemical-potential gradient. We describe the two leads with a BCS mean-field model and derive the current-bias characteristics for both particle and entropy transport. We compute the out of equilibrium steady-state currents by using the Keldysh formalism. In accordance with previous works in the literature, we confirm the well-known behavior for the particle current and extend the computation to the entropy current in the BCS regime. The entropy current shows an oscillatory behavior at low voltage in the ballistic junction limit. We analyze the results for a wide range of values of the junction's transparency. We also compare our findings with experimental results in cold atomic gases in the unitary regime.

cond-mat.quant-gas↗

Tomonaga-Luttinger liquid theory for one-dimensional attractive Fermi gases

The one-dimensional (1D) Yang-Gaudin model--an integrable $δ$-function interacting Fermi gas, serves as a paradigm in quantum many-body physics, encompassing phenomena from spin-charge separation to the Luther-Emery liquid. However, a consistent description of the Luther-Emery liquid and the Fulde-Ferrell-Larkin-Ovchinnikov (FFLO)-like pairing states in the 1D attractive Fermi gas remains elusive. In this work, we develop a universal Tomonaga-Luttinger liquid (TLL) theory to describe the FFLO state both for the case of weak and strong binding between fermions of opposite spins. We rigorously derive a low-energy effective Hamiltonian using bosonization, revealing the emergence of a two-component TLL: one exhibiting spin-charge coupling in the weak binding regime, and another featuring charge-charge separation in the strong binding regime. For the weak binding regime, we further derive renormalization-group equations for the sine-Gordon term in the spin sector and show that this term undergoes a relevant-irrelevant phase transition driven by the magnetic field. We further analyze the dynamical correlation functions of the FFLO pairing state based on the effective Hamiltonian we constructed. Finally, we discuss experiments using ultracold atoms to elucidate the Luther-Emery liquid behavior and the subtle phenomena of spin-charge coupling and charge-charge separation.

cond-mat.quant-gas↗