A neural network potential for the IRMOF series and its application for thermal and mechanical behaviors
Metal-organic frameworks (MOFs) with their exceptional porous and organized structures have been the subject of numerous applications. Predicting the bulk properties from atomistic simulations requires the most accurate force fields, which is still a major problem due to MOFs' hybrid structures...
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Published in | Physical chemistry chemical physics : PCCP Vol. 24; no. 19; pp. 11882 - 11897 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
England
Royal Society of Chemistry
18.05.2022
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Subjects | |
Online Access | Get full text |
ISSN | 1463-9076 1463-9084 1463-9084 |
DOI | 10.1039/d1cp05973d |
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Summary: | Metal-organic frameworks (MOFs) with their exceptional porous and organized structures have been the subject of numerous applications. Predicting the bulk properties from atomistic simulations requires the most accurate force fields, which is still a major problem due to MOFs' hybrid structures governed by covalent, ionic and dispersion forces. Application of
ab initio
molecular dynamics to such large periodic systems is thus beyond the current computational power. Therefore, alternative strategies must be developed to reduce computational cost without losing reliability. In this work, we construct a generic neural network potential (NNP) for the isoreticular metal-organic framework (IRMOF) series trained by PBE-D4/def2-TZVP reference data of MOF fragments. We confirmed the success of the resulting NNP on both fragments and bulk MOF structures by prediction of properties such as equilibrium lattice constants, phonon density of states and linker orientation. The RMSE values of energy and force for the fragments are only 0.0017 eV atom
−1
and 0.15 eV Å
−1
, respectively. The NNP predicted equilibrium lattice constants of bulk structures, even though not included in training, are off by only 0.2-2.4% from experimental results. Moreover, our fragment based NNP successfully predicts the phenylene ring torsional energy barrier, equilibrium bond distances and vibrational density of states of bulk MOFs. Furthermore, the NNP enables revealing the odd behaviors of selected MOFs such as the dual thermal expansion properties and the effect of mechanical strain on the adsorption of hydrogen and methane molecules. The NNP based molecular dynamics (MD) simulations suggest IRMOF-4 and IRMOF-7 to have positive-to-negative thermal expansion coefficients while the rest to have only negative thermal expansion at the studied temperatures of 200 K to 400 K. The deformation of the bulk structure by reduction of the unit cell volume has been shown to increase the volumetric methane uptake in IRMOF-1 but decrease the volumetric methane uptake in IRMOF-7 due to the steric hindrance. To the best of our knowledge, this study presents the first pre-trained model publicly available giving the opportunity for the researchers in the field to investigate different aspects of IRMOFs by performing large-scale simulation at the first-principles level of accuracy.
We construct a generic neural network potential (NNP) for IRMOF-n series trained by PBE-D4/def2-TZVP reference data of MOF fragments and identify bulk properties using NNP, much faster than DFT calculations. |
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Bibliography: | plots of IRMOF- T https://doi.org/10.1039/d1cp05973d V ( ) series, ASA and POAV change by stress applied structures of IRMOF-1 and IRMOF-7. Supplementary tables of thermal expansion coefficient calculations, equilibrium lattice parameters and thermal pressure coefficients. See DOI 1, 4, 6, 7, 10) fragments, uncertainty between NNPs, training and loss curves, histogram of energy errors, DFT and NNP produced energies of fragments, IRMOF-1 truncated structure used in torsional barrier, IRMOF-1 and IRMOF-7 vibrations' zoomed sections, ln Electronic supplementary information (ESI) available: Supplementary figures of IRMOF- n ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 content type line 23 |
ISSN: | 1463-9076 1463-9084 1463-9084 |
DOI: | 10.1039/d1cp05973d |