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Transformer variational wave functions for frustrated quantum spin systems
Luciano Loris Viteritti, Riccardo Rende, Federico Becca
TL;DR
Frustrated quantum spin systems pose challenges for variational wave functions because of their nontrivial ground-state sign structure, while fully connected RBMs scale poorly. This paper adapts the Vision Transformer into a complex-parameter variational wave function that mixes local and global operations. For the one-dimensional J1-J2 Heisenberg model, it reports excellent results across gapped and gapless phases, including agreement with DMRG correlations and dimer order.
Problem
Frustrated systems have nontrivial ground-state sign structures that challenge accurate variational wave functions, and fully connected RBMs scale poorly.
Source: p. 2Method
The paper adapts the Vision Transformer into a complex-parameter variational wave function that mixes local and global structures.
Source: pp. 1–2Results
The ViT state matches DMRG spin correlations at all distances in the unfrustrated model and shows excellent DMRG agreement across the three studied frustration ratios, reproducing dimer order.
Source: p. 4Takeaways & Limitations
The ViT state's mixture of local and global structures makes it flexible for describing quantum phases with both gapped and gapless spectra.
Source: p. 4
Abstract
from arXiv · showhide
The Transformer architecture has become the state-of-art model for natural language processing tasks and, more recently, also for computer vision tasks, thus defining the Vision Transformer (ViT) architecture. The key feature is the ability to describe long-range correlations among the elements of the input sequences, through the so-called self-attention mechanism. Here, we propose an adaptation of the ViT architecture with complex parameters to define a new class of variational neural-network states for quantum many-body systems, the ViT wave function. We apply this idea to the one-dimensional $J_1$-$J_2$ Heisenberg model, demonstrating that a relatively simple parametrization gets excellent results for both gapped and gapless phases. In this case, excellent accuracies are obtained by a relatively shallow architecture, with a single layer of self-attention, thus largely simplifying the original architecture. Still, the optimization of a deeper structure is possible and can be used for more challenging models, most notably highly-frustrated systems in two dimensions. The success of the ViT wave function relies on mixing both local and global operations, thus enabling the study of large systems with high accuracy.
Optimization of the variational wave function
The optimization minimizes the variational energy over the wave-function parameters using Stochastic Reconfiguration. Expectations are estimated by Monte Carlo sampling, and the procedure regularizes the optimization matrix to limit numerical instability.
Optimization of the variational wave function
- The optimization target is the variational energy, minimized with respect to the variational parameters.The energy is defined as the Hamiltonian expectation value in the variational state, normalized by its norm.Source: Optimization of the variational wave… · p. 7
- Stochastic Reconfiguration optimizes the variational energy by updating the variational parameters using forces and a learning rate.The method defines a computational-basis diagonal operator for each parameter.Source: Optimization of the variational wave… · p. 7
- The expectation values ⟨···⟩W, defined with respect to |ΨW(σ)|², are estimated stochastically using the Metropolis algorithm with a sample size of O(10^3 ÷ 10^4).Source: Optimization of the variational wave… · p. 7
- For L = 100, convergence takes O(10^2 ÷ 10^3) steps with learning rate η = 10^-2 ÷ 10^-3.The S-matrix is regularized by shifting its diagonal by ε, typically 10^-3 ÷ 10^-4, to prevent numerical instability when it is not invertible.Source: Optimization of the variational wave… · p. 7