aiqbench analysis
This paper presents an analog quantum simulation protocol using atomic lattices and Floquet dynamics to model four-body potentials in bosonic BFSS-like matrix quantum mechanics. By maintaining a constant number of control stages per cycle, the approach achieves polynomial scaling ($\mathcal{O}(N^3)$) for large-$N$ systems while enabling the study of strong-coupling holographic phases. The work offers a promising pathway for experimental realization of complex holographic physics without the circuit depth limitations of gate-based digital quantum computers.
Matrix Holography on an Optical Lattice
arXiv:2609.05613v1 Announce Type: cross Abstract: We propose an analog quantum-simulation protocol based on a lattice of atomic ensembles and time-averaged Floquet dynamics to construct the four-body potentials that typically appear in bosonic BFSS-like matrix quantum mechanics. In contrast to gate-based digital implementations requiring deep circuits, our approach generates the target model through a fixed set of control stages per Floquet cycle, keeping the number of consecutive unitaries constant with respect to the matrix size $N$. The principal scaling cost in our construction is given by the frequency range required to control the growing lattice. We show that this cost grows at most as $\mathcal{O}(N^3)$, giving a polynomial scaling route to large$-N$, attractive to experimental implementation. Additionally, we demonstrate that the coupling parameter can be tuned beyond $\mathcal{O}(1)$, enabling the simulation of strong-coupling physics necessary for holographic phases.
Abstract:We propose an analog quantum-simulation protocol based on a lattice of atomic ensembles and time-averaged Floquet dynamics to construct the four-body potentials that typically appear in bosonic BFSS-like matrix quantum mechanics. In contrast to gate-based digital implementations requiring deep circuits, our approach generates the target model through a fixed set of control stages per Floquet cycle, keeping the number of consecutive unitaries constant with respect to the matrix size $N$. The principal scaling cost in our construction is given by the frequency range required to control the growing lattice. We show that this cost grows at most as $\mathcal{O}(N^3)$, giving a polynomial scaling route to large$-N$, attractive to experimental implementation. Additionally, we demonstrate that the coupling parameter can be tuned beyond $\mathcal{O}(1)$, enabling the simulation of strong-coupling physics necessary for holographic phases.
High Energy Physics - Theory (hep-th); Quantum Gases (cond-mat.quant-gas); Atomic Physics (physics.atom-ph); Quantum Physics (quant-ph)
arXiv:2609.05613 [hep-th]
(or arXiv:2609.05613v1 [hep-th] for this version)
https://doi.org/10.48550/arXiv.2609.05613 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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Full text under the publisher's open licence · 238 words
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