2021/05/23 by Qiaohao Liang, Liang, Qiaohao, Aldair E. Gongora +29 · 16 citations
Computer Science · Materials Science · Physics and Astronomy · #Artificial intelligence #Bayesian optimization #Benchmarking #Computer science #Data Analysis #FOS: Computer and information sciences #FOS: Physical sciences #Gaussian #Gaussian process #Machine Learning (cs.LG) #Machine Learning and Algorithms #Machine Learning and Data Classification #Machine Learning in Materials Science #Machine learning #Materials Science (cond-mat.mtrl-sci) #Materials science #Physics #Selection (genetic algorithm) #Statistics and Probability (physics.data-an) #Surrogate model #Throughput #cond-mat.mtrl-sci #cs.LG #physics.data-an
paper · pdf · doi:10.48550/arxiv.2106.01309
published in arXiv (Cornell University) (Cornell University)
arxiv created 2021/05/23 · openalex publication_date 2021/05/23 · arxiv updated 2021/06/03 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
In the field of machine learning (ML) for materials optimization, active learning algorithms, such as Bayesian Optimization (BO), have been leveraged for guiding autonomous and high-throughput experimentation systems. However, very few studies have evaluated the efficiency of BO as a general optimization algorithm across a broad range of experimental materials science domains. In this work, we evaluate the performance of BO algorithms with a collection of surrogate model and acquisition function pairs across five diverse experimental materials systems, namely carbon nanotube polymer blends, silver nanoparticles, lead-halide perovskites, as well as additively manufactured polymer structures and shapes. By defining acceleration and enhancement metrics for general materials optimization objectives, we find that for surrogate model selection, Gaussian Process (GP) with anisotropic kernels (automatic relevance detection, ARD) and Random Forests (RF) have comparable performance and both outperform the commonly used GP without ARD. We discuss the implicit distributional assumptions of RF and GP, and the benefits of using GP with anisotropic kernels in detail. We provide practical insights for experimentalists on surrogate model selection of BO during materials optimization campaigns.