D. Mariscal, B. Djordjević, R. Anirudh, J. Jayaraman-Thiagarajan, E. Grace, R. Simpson, K. Swanson, T. C. Galvin, D. Mittelberger, J. Heebner, R. Muir, E. Folsom, M. P. Hill, S. Feister, E. Ito, K. Valdez-Sereno, J. J. Rocca, J. Park, S. Wang, R. Hollinger, R. Nedbailo, B. Sullivan, G. Zeraouli, A. Shukla, P. Turaga, A. Sarkar, B. Van Essen, S. Liu, B. Spears, P.-T. Bremer, T. Ma
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引用次数: 0
摘要
我们介绍了利用机器学习(ML)辅助优化框架研究参数空间趋势的进展,该参数空间由光谱成形、高强度、小功率级(8 J,45 fs)激光脉冲与固体靶相互作用所定义,并首次对预测趋势进行了基于模拟的概述。我们训练了一个包含不确定性量化的神经网络(NN),以预测激光与目标相互作用产生的热电子数量与脉冲整形参数的函数关系。该神经网络的预测结果可作为贝叶斯优化框架的基础函数,用于导航该空间。为了进行实验后评估,我们比较了两个独立的神经网络(NN)模型。其中一个完全基于实验数据,而另一个则仅在粒子入胞模拟中进行训练。回顾整个实验激光参数搜索空间的预测和观察趋势,我们发现两个 ML 模型都预测热电子生成的最大增幅约为 12%-18%;但在实验中并未观察到统计意义上的显著增强。直接比较 NN 模型,平均差异为 8.5%,最大差异为 30%。由于实验中镜头间的波动会影响观测结果,我们通过执行虚拟实验来评估优化框架的行为,这些虚拟实验改变了重复观测的数量和噪声水平。在此,我们讨论了这种框架对未来高重复率实验中自主探索平台的影响。
Toward machine-learning-assisted PW-class high-repetition-rate experiments with solid targets
We present progress in utilizing a machine learning (ML) assisted optimization framework to study the trends in a parameter space defined by spectrally shaped, high-intensity, petawatt-class (8 J, 45 fs) laser pulses interacting with solid targets and give the first simulation-based overview of predicted trends. A neural network (NN) incorporating uncertainty quantification is trained to predict the number of hot electrons generated by the laser–target interaction as a function of pulse shaping parameters. The predictions of this NN serve as the basis function for a Bayesian optimization framework to navigate this space. For post-experimental evaluation, we compare two separate neural network (NN) models. One is based solely on data from experiments, and the other is trained only on ensemble particle-in-cell simulations. Reviewing the predicted and observed trends across the experiment-capable laser parameter search space, we find that both ML models predict a maximal increase in hot electron generation at a level of approximately 12%–18%; however, no statistically significant enhancement was observed in experiments. On direct comparison of the NN models, the average discrepancy is 8.5%, with a maximum of 30%. Since shot-to-shot fluctuations in experiments affect the observations, we evaluate the behavior of our optimization framework by performing virtual experiments that vary the number of repeated observations and the noise levels. Here, we discuss the implications of such a framework for future autonomous exploration platforms in high-repetition-rate experiments.