Affiliation:
1. Physics Department, Temple University, Philadelphia, PA 19122, USA
2. Department of Chemistry, Rice University, Houston, TX 77251, USA
Abstract
Abstract
The errors in atomization energies (AE) of molecules have long been used to measure the
errors of wavefunction or density functional methods for electronic structure
calculations. In particular, the G3 set of Pople and collaborators (for sp-bonded
molecules from the first rows of the periodic table) has become a standard benchmark for
such methods. But the mean absolute error of AE tends to increase with increasing number
N
at of atoms in a molecule. In fact, AE is an extensive variable, which
diverges as N
at →∞. Here, as did Savin and Johnson 2015, we define an
intensive atomization energy, IAE = AE/N
at or atomization energy per atom, which
tends to the finite cohesive energy (per atom) of a large cluster or solid (N
at →∞). We find that the mean absolute error of the G3 molecular IAE from
accurate density functionals remains close to 1 kcal/mol as the average molecular
size increases. This makes it possible to estimate in advance the magnitude of the error in
AE for a molecule similar to most of those in the G3 set. It also allows us identify the
G3 “outlying molecules”, and to more directly compare the accuracy of a given functional
for different kinds of molecules (such as those containing transition-metal atoms) to that
for G3-type molecules, by removing the otherwise-uncontrolled size factor. Finally, we point
out that the familiar concept of “chemical accuracy” needs to be qualified.
Subject
Physical and Theoretical Chemistry
Cited by
14 articles.
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