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A critical comparison of MINDO/3, MNDO, AM1, and PM3 for a model problem: Carbon clusters C 2 ‐C 10 . An ad hoc reparametrization of MNDO well suited for the accurate prediction of their spectroscopic constants
Author(s) -
Martin J. M. L.,
François J. P.,
Gijbels R.
Publication year - 1991
Publication title -
journal of computational chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.907
H-Index - 188
eISSN - 1096-987X
pISSN - 0192-8651
DOI - 10.1002/jcc.540120107
Subject(s) - mndo , mindo , ab initio , chemistry , diatomic molecule , computational chemistry , standard enthalpy of formation , binding energy , atomic physics , ab initio quantum chemistry methods , molecular physics , physics , molecule , organic chemistry
Dissociation energies and potential energy surface features for the carbon clusters C 2 to C 10 are compared with ab initio or experimental results for the semiempirical methods MINDO/3, MNDO, AM1, and PM3. Quite surprisingly, MINDO/3 gives a rather good account of the various structures and electronic states, unlike the other three methods. MINDO/3 tends towards systematic overestimates of binding energies, the other methods to systematic gross underestimates. Reparametrization of the diatomic parameters α, β s , and β p for exact reproduction of the experimental data for C 3 results in much improved values for binding energies, but fails to correct the state splittings. Also reparametrizing U ss , U pp , ζ s , and ζ p to reproduce the ab initio linear‐rhombic energy difference in C 4 results in a much improved description of the other states. For the linear structures, computed harmonic frequencies with the latter parameters are in surprisingly good agreement with experimental or correlated ab initio data, where available; experimental values are consistently overestimated by about 40 cm −1 . Other results are comparable in quality to good ab initio treatments. The experimental IR bands at 2128 and 1892 cm −1 , formerly assigned to C 9 , should be reassigned to linear C 7 . The intense 1997 cm −1 feature almost certainly belongs to C 9 ; bands at 1952 and 1197 cm −1 both belong to linear C 6 . Tentative assignments of bands in the 1600–1850 cm −1 region to various cyclic structures of C 6 , C 8 , and C 10 have been made. As such, this suggests a new and promising procedure for the theoretical study of large molecules in general, and of large clusters in particular.