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dc.contributor.authorJankiewicz, Wojciechen_US
dc.contributor.authorPodeszwa, Rafalen_US
dc.contributor.authorWitek, Henryk A.en_US
dc.date.accessioned2019-04-02T06:00:27Z-
dc.date.available2019-04-02T06:00:27Z-
dc.date.issued2018-10-01en_US
dc.identifier.issn1549-9618en_US
dc.identifier.urihttp://dx.doi.org/10.1021/acs.jctc.8b00167en_US
dc.identifier.urihttp://hdl.handle.net/11536/148282-
dc.description.abstractWe demonstrate that the dispersion-corrected density functional theory (DFT-D) schemes fall short of predicting reliable three-body interaction energies. This concerns also a popular variant of DFT-D called the "many-body dispersion" (MBD) method, which might seem surprising in the light of the fact that its name contains the very phrase "many-body". The main reason for the inaccuracy of the three-body interaction energies in the DFT-D schemes can be attributed to internal deficiencies of the standard DFT functionals that the existing "-D" methods are incapable of correcting since the main problems emerge from the terms not related to the dispersion component. At present, it seems that none of the a posteriori dispersion techniques are able to predict accurately the total interaction energy for a supermolecular system together with its simultaneous decomposition into the many-body components. On the other hand, if one is interested only in the three-body interaction energies, we propose an adjustment to the MBD approach that achieves good accuracy in conjunction with the supermolecular MP2.en_US
dc.language.isoen_USen_US
dc.titleDispersion-Corrected DFT Struggles with Predicting Three-Body Interaction Energiesen_US
dc.typeArticleen_US
dc.identifier.doi10.1021/acs.jctc.8b00167en_US
dc.identifier.journalJOURNAL OF CHEMICAL THEORY AND COMPUTATIONen_US
dc.citation.volume14en_US
dc.citation.spage5079en_US
dc.citation.epage5089en_US
dc.contributor.department應用化學系zh_TW
dc.contributor.departmentDepartment of Applied Chemistryen_US
dc.identifier.wosnumberWOS:000447238500009en_US
dc.citation.woscount2en_US
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