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Quantum Entanglement in Neural Network States

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arxiv 1701.04844 v3 pith:3LJSGCOM submitted 2017-01-17 cond-mat.dis-nn cond-mat.quant-gasquant-ph

Quantum Entanglement in Neural Network States

classification cond-mat.dis-nn cond-mat.quant-gasquant-ph
keywords statesentanglementquantumlearningmachinemany-bodyrandomartificial
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Machine learning, one of today's most rapidly growing interdisciplinary fields, promises an unprecedented perspective for solving intricate quantum many-body problems. Understanding the physical aspects of the representative artificial neural-network states is recently becoming highly desirable in the applications of machine learning techniques to quantum many-body physics. Here, we study the quantum entanglement properties of neural-network states, with a focus on the restricted-Boltzmann-machine (RBM) architecture. We prove that the entanglement of all short-range RBM states satisfies an area law for arbitrary dimensions and bipartition geometry. For long-range RBM states we show by using an exact construction that such states could exhibit volume-law entanglement, implying a notable capability of RBM in representing efficiently quantum states with massive entanglement. We further examine generic RBM states with random weight parameters. We find that their averaged entanglement entropy obeys volume-law scaling and meantime strongly deviates from the Page-entropy of the completely random pure states. We show that their entanglement spectrum has no universal part associated with random matrix theory and bears a Poisson-type level statistics. Using reinforcement learning, we demonstrate that RBM is capable of finding the ground state (with power-law entanglement) of a model Hamiltonian with long-range interaction. In addition, we show, through a concrete example of the one-dimensional symmetry-protected topological cluster states, that the RBM representation may also be used as a tool to analytically compute the entanglement spectrum. Our results uncover the unparalleled power of artificial neural networks in representing quantum many-body states, which paves a novel way to bridge computer science based machine learning techniques to outstanding quantum condensed matter physics problems.

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Cited by 3 Pith papers

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    cond-mat.str-el 2026-03 unverdicted novelty 7.0

    Walsh complexity reveals that shallow additive neural quantum states require logarithmic depth to represent certain short-range entangled dimerized states with maximal parity spread.

  2. Projector, Neural, and Tensor-Network Representations of $\mathbb{Z}_N$ Cluster and Dipolar-cluster SPT States

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    Z_N cluster and dipolar-cluster SPT wavefunctions admit closed-form projector, neural, and tensor-product representations that generalize Z_2 constructions and yield a TPS benchmarked against MPS via DMRG.

  3. Ground state preparation of random all-to-all Hamiltonians using ADAPT-VQE

    quant-ph 2026-06 unverdicted novelty 4.0

    TETRIS-ADAPT-VQE achieves fidelities above 99.3% for SYK (N=20) and 99.9998% for SK (L=18) but requires large resources for SYK models.