Performance of a nonempirical density functional on molecules and hydrogen-bonded complexes
Journal Article
·
· Journal of Chemical Physics
- Temple Univ., Philadelphia, PA (United States); Department of Physics, Temple University, Philadelphia, Pennsylvania
- Temple Univ., Philadelphia, PA (United States); Kunming Univ. of Science and Technology, Kunming (China)
- Princeton Univ., Princeton, NJ (United States)
- The Univ. of Western Ontario, London, ON (Canada)
- Rice Univ., Houston, TX (United States)
- Temple Univ., Philadelphia, PA (United States)
Recently, Tao and Mo derived a meta-generalized gradient approximation functional based on a model exchange-correlation hole. In this work, the performance of this functional is assessed on standard test sets, using the 6-311++G(3df,3pd) basis set. These test sets include 223 G3/99 enthalpies of formation, 99 atomization energies, 76 barrier heights, 58 electron affinities, 8 proton affinities, 96 bond lengths, 82 harmonic vibrational frequencies, 10 hydrogen-bonded molecular complexes, and 22 atomic excitation energies. Here our calculations show that the Tao-Mo functional can achieve high accuracy for most properties considered, relative to the local spin-density approximation, Perdew-Burke-Ernzerhof, and Tao-Perdew-Staroverov-Scuseria functionals. In particular, it yields the best accuracy for proton affinities, harmonic vibrational frequencies, hydrogen-bond dissociation energies and bond lengths, and atomic excitation energies.
- Research Organization:
- Temple Univ., Philadelphia, PA (United States)
- Sponsoring Organization:
- USDOE; USDOE Office of Science (SC), Basic Energy Sciences (BES) (SC-22)
- Grant/Contract Number:
- SC0001474
- OSTI ID:
- 1474133
- Alternate ID(s):
- OSTI ID: 1336838
- Journal Information:
- Journal of Chemical Physics, Journal Name: Journal of Chemical Physics Journal Issue: 23 Vol. 145; ISSN 0021-9606
- Publisher:
- American Institute of Physics (AIP)Copyright Statement
- Country of Publication:
- United States
- Language:
- English
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