2023
DOI: 10.1103/physreva.108.063320
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Machine learning one-dimensional spinless trapped fermionic systems with neural-network quantum states

J. W. T. Keeble,
M. Drissi,
A. Rojo-Francàs
et al.
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Cited by 3 publications
(18 citation statements)
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“…The inputs to our network are the A positions of fermions in the system, x i , i = 1, …, A , and the output is the many-body wave function Ψ θ x 1 , …, x A in the log domain. The state depends on a series of network weights and biases, succinctly summarized by a variable θ of dimension N [7]. The network is composed of four core components: equivariant layers, generalized Slater matrices (GSMs), Gaussian log-envelope functions and a summed signed-log determinant function [46].…”
Section: (C) Neural Quantum States and Monte Carlo Samplingmentioning
confidence: 99%
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“…The inputs to our network are the A positions of fermions in the system, x i , i = 1, …, A , and the output is the many-body wave function Ψ θ x 1 , …, x A in the log domain. The state depends on a series of network weights and biases, succinctly summarized by a variable θ of dimension N [7]. The network is composed of four core components: equivariant layers, generalized Slater matrices (GSMs), Gaussian log-envelope functions and a summed signed-log determinant function [46].…”
Section: (C) Neural Quantum States and Monte Carlo Samplingmentioning
confidence: 99%
“…HF and CI results are displayed for reference, with horizontal green and orange dashed lines. CI results are displayed for A ≤ 5 and V 0 ≥ − 10 where we have access to converged results [7].…”
Section: (D) Improving the Scaling Estimationmentioning
confidence: 99%
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