Skip to content
aiqbench takeQuantum Computing

aiqbench analysis

This research establishes collectivity as a fundamental mechanism that constrains many-body quantum entanglement even in systems with strong nonlocal interactions, challenging the traditional reliance on spatial locality alone. By rigorously analyzing generic gapped Hamiltonians with power-law interactions, the study demonstrates how suppressed collective fluctuations can enforce polylogarithmic scaling bounds on entanglement entropy. These findings advance the theoretical understanding of entanglement limits, which is critical for optimizing error correction and scalability in future quantum computing architectures.
Sources coveringarXiv, Quantum Zeitgeist, electronicsweekly.com
What this isA model's reading of the article and related coverage, written for aiqbench. Not the publisher's words.

Collectivity limits quantum entanglement

arXiv2 min read

arXiv:2609.36113v1 Announce Type: new Abstract: Understanding what limits many-body quantum entanglement is a central problem in physics. Spatial locality has long provided a fundamental mechanism: correlations between a region and its complement must be mediated through a small spatial interface, thereby constraining their entanglement. Here we show that universal constraints on entanglement can persist even when interactions are strongly nonlocal, through collectivity: many weak interactions suppress collective quantum fluctuations while retaining a finite overall interaction scale. We establish this mechanism rigorously for generic gapped Hamiltonians with Kac-normalized power-law interactions $r^{-\alpha}$ on a $D$-dimensional lattice. For arbitrary bipartitions, we prove that the ground-state entanglement scales at most logarithmically with system size for $\alpha<D/2$ and subextensively for $D/2<\alpha<D$, due to suppressed collective fluctuations around individual sites. For spatially regular bipartitions with codimension-one boundaries, we show that collective suppression can be propagated to successively larger length scales through a renormalization-group construction. As a result, we prove that the entanglement bound improves to polylogarithmic scaling for $D/2<\alpha<(D+1)/2$, and remains parametrically stronger than the arbitrary-bipartition bound for $(D+1)/2<\alpha<D$. Together, these results reveal collectivity as a fundamental mechanism for constraining many-body entanglement alongside spatial locality.

Abstract:Understanding what limits many-body quantum entanglement is a central problem in physics. Spatial locality has long provided a fundamental mechanism: correlations between a region and its complement must be mediated through a small spatial interface, thereby constraining their entanglement. Here we show that universal constraints on entanglement can persist even when interactions are strongly nonlocal, through collectivity: many weak interactions suppress collective quantum fluctuations while retaining a finite overall interaction scale. We establish this mechanism rigorously for generic gapped Hamiltonians with Kac-normalized power-law interactions $r^{-\alpha}$ on a $D$-dimensional lattice. For arbitrary bipartitions, we prove that the ground-state entanglement scales at most logarithmically with system size for $\alpha<D/2$ and subextensively for $D/2<\alpha<D$, due to suppressed collective fluctuations around individual sites. For spatially regular bipartitions with codimension-one boundaries, we show that collective suppression can be propagated to successively larger length scales through a renormalization-group construction. As a result, we prove that the entanglement bound improves to polylogarithmic scaling for $D/2<\alpha<(D+1)/2$, and remains parametrically stronger than the arbitrary-bipartition bound for $(D+1)/2<\alpha<D$. Together, these results reveal collectivity as a fundamental mechanism for constraining many-body entanglement alongside spatial locality.

Quantum Physics (quant-ph); Disordered Systems and Neural Networks (cond-mat.dis-nn); Statistical Mechanics (cond-mat.stat-mech); Mathematical Physics (math-ph)

arXiv:2609.36113 [quant-ph]

(or arXiv:2609.36113v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2609.36113 arXiv-issued DOI via DataCite (pending registration)

Full text under the publisher's open licence · 214 words

Related coverage