具有密度函数精度的自由钠簇的机器学习势能面:在熔化中的应用

Balasaheb J. Nagare, Sajeev Chacko, Dilip. G. Kanhere
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引用次数: 0

摘要

基于高斯过程回归的高斯近似势已被用于开发具有密度泛函精度的自由钠团簇的机器学习原子间势。训练数据是使用VASP包中实现的密度泛函方法,从为N = 40 - 200的大小范围内的聚类计算的超过100,000个数据点的大样本中生成的。已经开发了两个模型,模型M1仅使用N=55的数据,而模型M2使用来自较大集群的附加数据。这些模型的目的是利用分子动力学计算热力学性质。因此,特别注意改进力的拟合。有趣的是,对于M1和M2两种模型,通过仔细选择较少数量的数据点,即分别为1,900和1,300个配置,可以获得最佳拟合。虽然仅使用Na55的数据可以获得很好的拟合,但需要来自较大簇的额外数据点才能获得更大尺寸的能量和力的更好精度。令人惊讶的是,通过在每个集群中增加大约50个数据点,M1模型可以得到显著改进。这两种模型都被用于计算Na55和Na147的热容,并得到了大约40种尺寸为N = 147、200、201和252的大簇的异构体。计算的熔化温度与实验测量的熔化温度非常吻合。这些异构体的几何形状经DFT进一步优化后,DFT结果与我们的模型之间能量的平均绝对误差约为7 meV/原子或更小。在几乎所有情况下,原子间键长度的误差估计在2%以下。
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Machine-Learned Potential Energy Surfaces for Free Sodium Clusters with Density Functional Accuracy: Applications to Melting
Gaussian Process Regression-based Gaussian Approximation Potential has been used to develop machine-learned interatomic potentials having density-functional accuracy for free sodium clusters. The training data was generated from a large sample of over 100,000 data points computed for clusters in the size range of N = 40 - 200, using the density-functional method as implemented in the VASP package. Two models have been developed, model M1 using data for N=55 only, and model M2 using additional data from larger clusters. The models are intended for computing thermodynamic properties using molecular dynamics. Hence, particular attention has been paid to improve the fitting of the forces. Interestingly, it turns out that the best fit can be obtained by carefully selecting a smaller number of data points viz. 1,900 and 1,300 configurations, respectively, for the two models M1 and M2. Although it was possible to obtain a good fit using the data of Na55 only, additional data points from larger clusters were needed to get better accuracies in energies and forces for larger sizes. Surprisingly, the model M1 could be significantly improved by adding about 50 data points per cluster from the larger sizes. Both models have been deployed to compute the heat capacities of Na55 and Na147 and to obtain about 40 isomers for larger clusters of sizes N = 147, 200, 201, and 252. There is an excellent agreement between the computed and experimentally measured melting temperatures. The geometries of these isomers when further optimized by DFT, the mean absolute error in the energies between DFT results and those of our models is about 7 meV/atom or less. The errors in the interatomic bond lengths are estimated to be below 2% in almost all the cases.
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