All the semiempirical methods contain sets of parameters. Atomic and diatomic parameters exist in PM6, while MNDO, AM1, PM3, and MNDO-d use only single-atom parameters. Not all parameters are optimized for all methods; for example, in MNDO and AM1 the two electron one center integrals are normally taken from atomic spectra. In the following Table, parameters optimized for a given method are indicated by '*'. A '+' indicates that the value of the parameter was obtained from experiment (not optimized). Where neither symbol is given, the associated parameter is not used in that method.
Table of Parameters
| Parameter | Description | Units |
MNDO |
AM1 |
PM3 |
PM6 |
| Uss, Upp, Udd | s, p, and d atomic orbital one-electron one-center integrals |
eV |
* |
* |
* |
* |
| βs, βp, and βd | s, p, and d atomic orbital
one-electron two-center resonance integral terms |
eV |
* |
* |
* |
* |
| ξs, ξp, and ξd | s, p, and d Slater atomic orbital exponent | bohr-1 |
* |
* |
* |
* |
| ξsn, ξpn, and ξdn | s, p, and d Slater atomic orbital internal exponent | bohr-1 |
* |
* |
* |
* |
| αA | Atom A core-core repulsion term | Å-1 |
* |
* |
* |
|
| αAB | Atoms A and B core-core repulsion term | Å-1 |
|
|
|
* |
| Gss | s-s atomic orbital one
center two electron repulsion integral |
eV |
+ |
+ |
* |
* |
| Gsp | s-p atomic orbital one
center two electron repulsion integral |
eV |
+ |
+ |
* |
* |
| Gpp | p-p atomic orbital one
center two electron repulsion integral |
eV |
+ |
+ |
* |
* |
| Gp2 | p-p' atomic orbital one
center two electron repulsion integral |
eV |
+ |
+ |
* |
* |
| Hsp | s-p atomic orbital
one-center two-electron exchange integral |
eV |
+ |
+ |
* |
* |
| KnA or anA | A Gaussian multiplier for nth Gaussian of atom A |
none |
|
* |
* |
* |
| LnA or bnA | A Gaussian exponent multiplier Gaussian of atom A |
Å-2 |
|
* |
* |
* |
| MnA or cnA | A Radius of center of nth Gaussian of atom A |
Å |
|
* |
* |
* |