dftd4-fitset

Benchmark sets used in the parametrisation of the DFT-D4 method

https://github.com/dftd4/dftd4-fitset

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Benchmark sets used in the parametrisation of the DFT-D4 method

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Created over 7 years ago · Last pushed over 3 years ago
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  • Name: DFT-D4
  • Login: dftd4
  • Kind: organization

A Generally Applicable Atomic-Charge Dependent London Dispersion Correction.

Citation (citation.bib)

@article{NCIBLIND10,
   author = {DeCarlos E. Taylor and J{\'a}nos G. {\'A}ngy{\'a}n and Giulia Galli and Cui Zhang and Francois Gygi and Kimihiko Hirao and Jong Won Song and Kar Rahul and O. Anatole von Lilienfeld and Rafa{\l} Podeszwa and Ireneusz W. Bulik and Thomas M. Henderson and Gustavo E. Scuseria and Julien Toulouse and Roberto Peverati and Donald G. Truhlar and Krzysztof Szalewicz},
   title = {Blind test of density-functional-based methods on intermolecular interaction energies},
   journal = {J. Chem. Phys.},
   volume = {145},
   number = {12},
   pages = {124105},
   year = {2016},
   doi = {10.1063/1.4961095},
   URL = {https://doi.org/10.1063/1.4961095},
   eprint = {https://doi.org/10.1063/1.4961095}
}
@article{S22x5,
   author = {Gr{\'a}fov{\'a}, Lucie and Pito{\v n}{\'a}k, Michal and {\v R}ez{\'a}{\v c}, Jan and Hobza, Pavel},
   title = {Comparative Study of Selected Wave Function and Density Functional Methods for Noncovalent Interaction Energy Calculations Using the Extended S22 Data Set},
   journal = {J. Chem. Theory Comput.},
   volume = {6},
   number = {8},
   pages = {2365-2376},
   year = {2010},
   doi = {10.1021/ct1002253},
   note ={PMID: 26613492},
   URL = {https://doi.org/10.1021/ct1002253},
   eprint = {https://doi.org/10.1021/ct1002253}
}
@article{S66x8_geometries,
   author = {{\v R}ez{\'a}{\v c}, Jan and Riley, Kevin E. and Hobza, Pavel},
   title = {S66: A Well-balanced Database of Benchmark Interaction Energies Relevant to Biomolecular Structures},
   journal = {J. Chem. Theory Comput.},
   volume = {7},
   number = {8},
   pages = {2427-2438},
   year = {2011},
   doi = {10.1021/ct2002946},
   note ={PMID: 21836824},
   URL = {https://doi.org/10.1021/ct2002946},
   eprint = {https://doi.org/10.1021/ct2002946}
}
@article{S66x8_energies,
    author ="Santra, Golokesh and Semidalas, Emmanouil and Mehta, Nisha and Karton, Amir and Martin, Jan M. L.",
    title  ="S66x8 noncovalent interactions revisited: new benchmark and performance of composite localized coupled-cluster methods",
    journal  ="Phys. Chem. Chem. Phys.",
    year  ="2022",
    volume  ="24",
    issue  ="41",
    pages  ="25555-25570",
    publisher  ="The Royal Society of Chemistry",
    doi  ="10.1039/D2CP03938A",
    url  ="http://dx.doi.org/10.1039/D2CP03938A",
    abstract  ="The S66x8 noncovalent interactions benchmark has been re-evaluated at the “sterling silver” level{,} using explicitly correlated MP2-F12 near the complete basis set limit{,} CCSD(F12*)/aug-cc-pVTZ-F12{,} and a (T) correction from conventional CCSD(T)/sano-V{D{,}T}Z+ calculations. The revised reference values differ by 0.1 kcal mol−1 RMS from the original Hobza benchmark and its revision by Brauer et al.{,} but by only 0.04 kcal mol−1 RMS from the “bronze” level data in Kesharwani et al.{,} Aust. J. Chem.{,} 2018{,} 71{,} 238–248. We then used these to assess the performance of localized-orbital coupled cluster approaches with and without counterpoise corrections{,} such as PNO-LCCSD(T) as implemented in MOLPRO{,} DLPNO-CCSD(T1) as implemented in ORCA{,} and LNO-CCSD(T) as implemented in MRCC{,} for their respective “Normal”{,} “Tight”{,} and “very Tight” settings. We also considered composite approaches combining different basis sets and cutoffs. Furthermore{,} in order to isolate basis set convergence from domain truncation error{,} for the aug-cc-pVTZ basis set we compared PNO{,} DLPNO{,} and LNO approaches with canonical CCSD(T). We conclude that LNO-CCSD(T) with veryTight criteria performs very well for “raw” (CP-uncorrected){,} but struggles to reproduce counterpoise-corrected numbers even for veryveryTight criteria: this means that accurate results can be obtained using either extrapolation from basis sets large enough to quench basis set superposition error (BSSE) such as aug-cc-pV{Q{,}5}Z{,} or using a composite scheme such as Tight{T{,}Q} + 1.11[vvTight(T) − Tight(T)]. In contrast{,} PNO-LCCSD(T) works best with counterpoise{,} while performance with and without counterpoise is comparable for DLPNO-CCSD(T1). Among more economical methods{,} the highest accuracies are seen for dRPA75-D3BJ{,} ωB97M-V{,} ωB97M(2){,} revDSD-PBEP86-D4{,} and DFT(SAPT) with a TDEXX or ATDEXX kernel."
}

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