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Neural Quantum States for Light Nuclei with Chiral Two- and Three-Body Interactions

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arxiv 2505.11442 v2 pith:L5RT2RKR submitted 2025-05-16 nucl-th

classification nucl-th
keywords carlomontenucleivariationalwavefunctionlightneural
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

Finding high-quality trial wave functions for quantum Monte Carlo calculations of light nuclei requires a strong intuition for modeling the interparticle correlations as well as large computational resources for exploring the space of variational parameters. Moreover, for systems with three-body interactions, the wave function should account for many-body effects beyond simple pairwise correlations. In this work, we design neural networks that efficiently incorporate these factors to generate expressive wave function Ans\"atze for light nuclei using variational Monte Carlo. Our neural-network approach for $A=3$ nuclei can capture, already at the level of variational Monte Carlo, the overwhelming majority of the ground-state energy estimated by Green's Function Monte Carlo (GFMC). It achieves a ground-state energy within $0.45\%$ of the GFMC result for $^3\mathrm{H}$ using the softest chiral interaction, representing a substantial improvement over standard variational Monte Carlo, which exhibits a $3.7\%$ deviation. The result indicates the potential of neural networks to construct effective trial wave functions for quantum Monte Carlo calculations.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Zemach radii and nuclear structure effects in hyperfine splitting of Lithium

    nucl-th 2025-09 conditional novelty 6.0 of 10

    Nuclear polarizability, enhanced in odd-odd nuclei by spin-isospin symmetry, explains the Zemach radius discrepancy between effective and elastic values in 6Li, 7Li, 2H, and 3He.

  2. Kolmogorov-Arnold Wavefunctions

    nucl-th 2025-06 conditional novelty 6.0 of 10

    KAN-based trial wavefunctions reach about 1 percent ground-state energy accuracy for one-dimensional trapped bosons at roughly 10 times lower cost per training step than MLP-based wavefunctions, aided by a transferabl...

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