具有受限玻尔兹曼机波函数的Bose-Hubbard模型相图重建

Vladimir Vargas-Calderón, H. Vinck-Posada, F. A. Gonz'alez
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引用次数: 4

摘要

最近,利用神经量子态来描述多体和少体问题的基态,由于其高表达性和处理棘手的大希尔伯特空间的能力而越来越受欢迎。特别是,基于变分蒙特卡罗的方法已被证明在描述玻色子系统的物理方面是成功的,例如玻色-哈伯德模型。然而,该技术尚未在玻色-哈伯德模型的参数空间上进行系统的测试,特别是在莫特绝缘体和超流体相之间的边界上。在这项工作中,我们用一个受限玻尔兹曼机给出的试波函数来评估变分蒙特卡罗在其参数空间的几个点上再现玻色-哈伯德模型的量子基态的能力。为了对该技术进行基准测试,我们将其结果与通过对小一维链进行精确对角化得到的基态进行了比较。总的来说,我们发现学习到的基态正确地估计了许多观测值,高度地再现了第一个莫特叶的相图和第二个莫特叶的部分相图。然而,我们发现每当系统在激励流形之间转换时,该技术就会受到挑战,因为在这些边界处不能正确地学习基态。尽管如此,我们提出了一种方法来丢弃在基态中学习到的噪声概率,这提高了该方法产生的结果的质量。
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Phase Diagram Reconstruction of the Bose–Hubbard Model with a Restricted Boltzmann Machine Wavefunction
Recently, the use of neural quantum states for describing the ground state of many- and few-body problems has been gaining popularity because of their high expressivity and ability to handle intractably large Hilbert spaces. In particular, methods based on variational Monte Carlo have proven to be successful in describing the physics of bosonic systems such as the Bose-Hubbard model. However, this technique has not been systematically tested on the parameter space of the Bose-Hubbard model, particularly at the boundary between the Mott insulator and superfluid phases. In this work, we evaluate the capabilities of variational Monte Carlo with a trial wavefunction given by a Restricted Boltzmann Machine to reproduce the quantum ground state of the Bose-Hubbard model on several points of its parameter space. To benchmark the technique, we compare its results to the ground state found through exact diagonalization for small one-dimensional chains. In general, we find that the learned ground state correctly estimates many observables, reproducing to a high degree the phase diagram for the first Mott lobe and part of the second one. However, we find that the technique is challenged whenever the system transitions between excitation manifolds, as the ground state is not learned correctly at these boundaries. Nonetheless, we propose a method to discard noisy probabilities learned in the ground state, which improves the quality of the results produced by the method.
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