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Physical review. E

Learning the Renyi entropy of multiple disjoint intervals in transverse-field quantum Ising models with a restricted Boltzmann machine

Han-Qing Shi, Hai-Qing Zhang

Published Nov 17, 2025• 0 citations
Publisher

Abstract

Renyi entropy with multiple disjoint intervals are computed from the improved swapping operations by two methods: One is from the direct diagonalization of the Hamiltonian and the other one is from the state-of-the-art machine learning method with neural networks. We use the paradigmatic transverse-field Ising model in one dimension to demonstrate the strategy of the improved swapping operation. In particular, we study the second Renyi entropy with two, three, and four disjoint intervals. We find that the results from the above two methods match each other very well within errors, which indicates that the machine learning method is applicable for calculating the Renyi entropy with multiple disjoint intervals. Moreover, as the magnetic field increases, the Renyi entropy grows as well until the system arrives at the critical point of the phase transition. However, as the magnetic field exceeds the critical value, the Renyi entropy will decrease since the system enters the paramagnetic phase. Overall, these results match the theoretical predictions very well and demonstrate the high accuracy of the machine learning methods with neural networks.

DOI
10.1103/b8xy-nq85

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•Jan 1, 2018•0 citations
Renyi entropy with multiple disjoint intervals are computed from the improved swapping operations by two methods: One is from the direct diagonalization of the Hamiltonian and the other one is from the state-of-the-art machine learning method with neural networks. We use the paradigmatic transverse-field Ising model in one dimension to demonstrate the strategy of the improved swapping operation. In particular, we study the second Renyi entropy with two, three, and four disjoint intervals. We find that the results from the above two methods match each other very well within errors, which indicates that the machine learning method is applicable for calculating the Renyi entropy with multiple disjoint intervals. Moreover, as the magnetic field increases, the Renyi entropy grows as well until the system arrives at the critical point of the phase transition. However, as the magnetic field exceeds the critical value, the Renyi entropy will decrease since the system enters the paramagnetic phase. Overall, these results match the theoretical predictions very well and demonstrate the high accuracy of the machine learning methods with neural networks.
Renyi entropy with multiple disjoint intervals are computed from the improved swapping operations by two methods: one is from the direct diagonalization of the Hamiltonian and the other one is from the state-of-the-art machine learning method with neural networks. We use the paradigmatic transverse-field Ising model in one-dimension to demonstrate the strategy of the improved swapping operation. In particular, we study the second Renyi entropy with two, three and four disjoint intervals. We find that the results from the above two methods match each other very well within errors, which indicates that the machine learning method is applicable for calculating the Renyi entropy with multiple disjoint intervals. Moreover, as the magnetic field increases, the Renyi entropy grows as well until the system arrives at the critical point of the phase transition. However, as the magnetic field exceeds the critical value, the Renyi entropy will decrease since the system enters the paramagnetic phase. Overall, these results match the theoretical predictions very well and demonstrate the high accuracy of the machine learning methods with neural networks.
We propose a universal approach to compute the Renyi entropy with generically multiple disjoint intervals from the swapping operations. The proposal is grounded in our observation that there is a striking similarity between the replica trick utilized in quantum field theory and the process of swapping operations. Consequently, the Renyi entropy of multiple disjoint intervals can be obtained by evaluating the expectation values of the swapping operator. As an application, we use our proposal to study the Renyi entropy of a one-dimensional transverse-field Ising model with two, three and four disjoint intervals. In particular, as the system is at the critical point, our results of the Renyi entropy are consistent with the analytical results from the conformal field theory. Remarkably, our approach can go beyond the critical regime where the analytical methods from conformal field theory can not apply.
Abstract We study the Rényi entropy in a one-dimensional transverse-field quantum Ising model by virtue of the machine learning methods with neural networks. The Rényi entropy is investigated both in the static ground state and in the dynamical state after a linear quench, by employing a swapping operator acting on the states prepared from the neural networks. In the ground state, the behavior of Rényi entropy can unveil the critical point from paramagnetic to ferromagnetic phase. At the critical point, the relation between the Rényi entropy and the subsystem size from the machine learning method satisfies the predictions from conformal field theory. In the quenching dynamics, coherent oscillations of the Rényi entropy are observed after the end of the quench. These oscillations have universal frequencies stem from the superpositions of the excited states. More importantly, an asymptotic scaling of the reduced Rényi entropy is observed, implying a novel length scale away from the critical point.
We compute the Renyi entropy in a one-dimensional transverse-field quantum Ising model by employing a swapping operator acting on the states which are prepared from the neural network methods. In the static ground state, Renyi entropy can uncover the critical point of the quantum phase transition from paramagnetic to ferromagnetic. At the critical point, the relation between the Renyi entropy and the subsystem size satisfies the predictions from conformal field theory. In the dynamical case, we find coherent oscillations of the Renyi entropy after the end of the linear quench. These oscillations have universal frequencies which may come from the superpositions of excited states. The asymptotic form of the Renyi entropy implies a new length scale away from the critical point. This length scale is also verified by the overlap of the reduced Renyi entropy against the dimensionless subsystem size.
We study the statistical physics of the classical Ising model in the so-called α -Rényi ensemble, a finite-temperature thermal state approximation that minimizes a modified free energy based on the α -Rényi entropy. We begin by characterizing its critical behavior in mean-field theory in different regimes of the Rényi index α . Next, we re-introduce correlations and consider the model in one and two dimensions, presenting analytical arguments for the former and devising a Monte Carlo approach to the study of the latter. Remarkably, we find that while mean-field predicts a continuous phase transition below a threshold index value of α ∼ 1.303 and a first-order transition above it, the Monte Carlo results in two dimensions point to a continuous transition at all α . We conclude by performing a variational minimization of the α -Rényi free energy using a recurrent neural network (RNN) where we find that the RNN performs well in two dimensions when compared to the Monte Carlo simulations. Our work highlights the potential opportunities and limitations associated with the use of the α -Rényi ensemble formalism in probing the thermodynamic equilibrium properties of classical and quantum systems.
Lately, there has been an extensive state-of-the-art research in Machine Learning methods, due to their important features such as universality in approximations and dimensional reduction. In this way, the present work aims at exploiting these properties of Machine Learning on physical many-body problems, in which a restricted Boltzmann Machine (RBM) is trained with quantum Monte Carlo data to best represent the ground state of an N spin system under the transverse field Ising model Hamiltonian in one dimension. During the path coursed along the development of this project, we first review classical well-implemented methods such as the single-layer perceptron, multi-layer perceptron for the XOR problem with back-propagation algorithm, discrete Hopfield network for pattern reconstruction, continuous Hopfield network with Simulated Annealing for solving the traveling salesman problem with 10 cities and the Boltzmann machine for feature extraction. Then, we review a few aspects of what is called a Quantum Boltzmann Machine and the basics of the transverse field Ising model. Finally, we train an RBM consisting of N visible neurons, hidden density neurons alpha=M/N=2 and 1-step contrastive divergence (CD_1), by minimizing the Kullbach-Liebler divergence of the RBM and the training data set coming from the algorithmic variant of quantum Monte Carlo, known as discrete Path-Integral Monte Carlo. For this last step, we use Trotter-Suzuki decomposition with m Trotter slices and the Wolff-s cluster algorithm. After training the RBM, we calculate magnetic observables based on the RBM-s wave-function such as longitudinal and transverse magnetization, for different values of transverse field and we do an estimation of the critical field at which the transverse Ising model system suffers a quantum phase transition from ferromagnet to paramagnet