论文标题
在未观察到的条件下进行的光学晶格实验,并通过生成的对抗深度学习
Optical lattice experiments at unobserved conditions and scales through generative adversarial deep learning
论文作者
论文摘要
机器学习为研究多体系统的实验实现提供了一种新颖的途径,并已被证明在分析超低量子气体实验数据的性质方面被证明是成功的。我们在这里表明,深度学习在建模这种实验数据分布的更具挑战性的任务中取得了成功。我们的生成模型(Rugan)能够生成掺杂的二维费米 - 哈伯德模型的快照,这些模型与先前报道的实验实现无法区分。重要的是,它能够在没有观察到任何实验数据的条件下准确生成快照,例如在较高的掺杂值下。最重要的是,我们的生成模型从小规模示例中提取相关模式,并可以使用它们以更大尺寸的新配置来构建新的配置,以作为目前在实验上无法访问的尺度上观察的先驱。我们的模型创建的快照 - 实际上是无成本的 - 非常有用,因为它们可以在未经实验探索的条件下进行定量测试新的理论发展,参数化现象学模型或培训其他,更多数据密集型机器学习方法。我们为在未观察到的条件下可观察到的实验性可观察物提供了预测,并根据现代理论框架进行基准测试。我们在这里开发的深度学习方法广泛适用,可用于对平衡和非平衡物理系统的有效大规模模拟。
Machine learning provides a novel avenue for the study of experimental realizations of many-body systems, and has recently been proven successful in analyzing properties of experimental data of ultracold quantum gases. We here show that deep learning succeeds in the more challenging task of modelling such an experimental data distribution. Our generative model (RUGAN) is able to produce snapshots of a doped two-dimensional Fermi-Hubbard model that are indistinguishable from previously reported experimental realizations. Importantly, it is capable of accurately generating snapshots at conditions for which it did not observe any experimental data, such as at higher doping values. On top of that, our generative model extracts relevant patterns from small-scale examples and can use these to construct new configurations at a larger size that serve as a precursor to observations at scales that are currently experimentally inaccessible. The snapshots created by our model---which come at effectively no cost---are extremely useful as they can be employed to quantitatively test new theoretical developments under conditions that have not been explored experimentally, parameterize phenomenological models, or train other, more data-intensive, machine learning methods. We provide predictions for experimental observables at unobserved conditions and benchmark these against modern theoretical frameworks. The deep learning method we develop here is broadly applicable and can be used for the efficient large-scale simulation of equilibrium and nonequilibrium physical systems.