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arXiv:1902.07006 · Physical review. B./Physical review. B

Constructing neural stationary states for open quantum many-body systems

Nobuyuki Yoshioka, Ryusuke Hamazaki

Published Jun 28, 2019• 180 citations
arXivHTMLPDF

Abstract

A theoretical exploration of exotic properties in open quantum many-body systems requires an efficient search of the nonequillibrum stationary states. Aiming to accelerate the process, the authors develop here a variational method, in which the ansatz for the mixed states is based on the restricted Boltzmann machine, motivated by its high expressive power shown in various recent works. It is demonstrated that the ansatz successfully simulates dissipative spin systems both in one and two dimensions.

DOI
10.1103/physrevb.99.214306

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A theoretical exploration of exotic properties in open quantum many-body systems requires an efficient search of the nonequillibrum stationary states. Aiming to accelerate the process, the authors develop here a variational method, in which the ansatz for the mixed states is based on the restricted Boltzmann machine, motivated by its high expressive power shown in various recent works. It is demonstrated that the ansatz successfully simulates dissipative spin systems both in one and two dimensions.
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Abstract In this work we apply deep neural networks to find the non-equilibrium steady state solution to correlated open quantum many-body systems. Motivated by the ongoing search to find more powerful representations of (mixed) quantum states, we design a simple prototypical convolutional neural network and show that parametrizing the density matrix directly with more powerful models can yield better variational ansatz functions and improve upon results reached by neural density operator based on the restricted Boltzmann machine. Hereby we give up the explicit restriction to positive semi-definite density matrices. However, this is fulfilled again to good approximation by optimizing the parameters. The great advantage of this approach is that it opens up the possibility of exploring more complex network architectures that can be tailored to specific physical properties. We show how translation invariance can be enforced effortlessly and reach better results with fewer parameters. We present results for the dissipative one-dimensional transverse-field Ising model and a two-dimensional dissipative Heisenberg model compared to exact values.
We propose a neural-network variational quantum algorithm to simulate the time evolution of quantum many-body systems.Based on a modified restricted Boltzmann machine (RBM) wave function ansatz, the proposed algorithm can be efficiently implemented in near-term quantum computers with low measurement cost.Using a qubit recycling strategy, only one ancilla qubit is required to represent all the hidden spins in an RBM architecture.The variational algorithm is extended to open quantum systems by employing a stochastic Schrödinger equation approach.Numerical simulations of spin-lattice models demonstrate that our algorithm is capable of capturing the dynamics of closed and open quantum many-body systems with high accuracy without suffering from the vanishing gradient (or "barren plateau") issue for the considered system sizes.
An artificial neural network (ANN) with the restricted Boltzmann machine (RBM) architecture was recently proposed as a versatile variational quantum many-body wave function. In this work we provide physical insights into the performance of this ansatz. We uncover the connection between the structure of the RBM and perturbation series, which explains the excellent precision achieved by the RBM ansatz in certain simple models, demonstrated in G. Carleo and M. Troyer [Science 355, 602 (2017)]. Based on this relation, we improve the numerical algorithm to achieve a better performance of the RBM in cases where local minima complicate the convergence to the global one. Furthermore, we study the performance of a sparse RBM for approximating ground states of random, translationally invariant models in one dimension, as well as random matrix-product states. We find that the error in approximating such states exhibits a broad distribution and shows a positive correlation with the entanglement properties of the targeted state.
Artificial neural netwokrs have proven to be a powerful tool with applications in various fields: from data processing and optical character recognition to traffic control or prediction of dynamic systems evolution. Recently, they have demonstrated to be a promising approach to solving quantum mechanical spin systems where neural network is used as an Ansatz representing the wave function. In the case of Heisenberg model, an architecture called restricted Boltzmann machine was successful, thus in this work, we are going to focus on its generalization, J1-J2 model in one as well as two dimensions, in order to find out whether restricted Boltzmann machines can be efficiently used also for frustrated spin systems.
Abstract The variational wave functions based on neural networks have recently started to be recognized as a powerful ansatz to represent quantum many-body states accurately. In order to show the usefulness of the method among all available numerical methods, it is imperative to investigate the performance in challenging many-body problems for which the exact solutions are not available. Here, we construct a variational wave function with one of the simplest neural networks, the restricted Boltzmann machine (RBM), and apply it to a fundamental but unsolved quantum spin Hamiltonian, the two-dimensional J 1 – J 2 Heisenberg model on the square lattice. We supplement the RBM wave function with quantum-number projections, which restores the symmetry of the wave function and makes it possible to calculate excited states. Then, we perform a systematic investigation of the performance of the RBM. We show that, with the help of the symmetry, the RBM wave function achieves state-of-the-art accuracy both in ground-state and excited-state calculations. The study shows a practical guideline on how we achieve accuracy in a controlled manner.