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arxiv: 1612.07805 · v1 · pith:LINNDEPCnew · submitted 2016-12-22 · ❄️ cond-mat.quant-gas · quant-ph

Entanglement and spin-squeezing without infinite-range interactions

classification ❄️ cond-mat.quant-gas quant-ph
keywords alphainteractionssystemsinfinite-rangesqueezingcontextexperimentalsize
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Infinite-range interactions are known to facilitate the production of highly entangled states with applications in quantum information and metrology. However, many experimental systems have interactions that decay with distance, and the achievable benefits in this context are much less clear. Combining recent exact solutions with a controlled expansion in the system size, we analyze quench dynamics in Ising models with power-law ($1/r^{\alpha}$) interactions in $D$ dimensions, thereby expanding the understanding of spin squeezing into a broad and experimentally relevant context. In spatially homogeneous systems, we show that for small $\alpha$ the scaling of squeezing with system size is identical to the infinite-range ($\alpha=0$) case. This indifference to the interaction range persists up to a critical value $\alpha=2D/3$, above which squeezing degrades continuously. Boundary-induced inhomogeneities present in most experimental systems modify this picture, but it nevertheless remains qualitatively correct for finite-sized systems.

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Cited by 2 Pith papers

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    Scalable spin squeezing on arbitrary quantum networks is achievable when the interaction graph's spectral dimension meets universal criteria and the system lies below the xy-ferromagnetic symmetry breaking transition.

  2. Universal Spin Squeezing Dynamical Phase Transitions across Lattice Geometries, Dimensions, and Microscopic Couplings

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    The dynamical squeezing phase transition in bilayer XXZ spin models is universal across lattice geometries and interlayer coupling rescalings, with a new sub-linear scaling for short-range interactions.