Abstract
Potential energy curves of a single electron moving in the joint Coulomb field of two fixed nuclei of equal arbitrary charge, Z, have been calculated exactly using a scaling relationship derived in an earlier paper. The resulting potential curves display some interesting features. For Z<1 the 2 pσ "antibonding" orbital becomes "bonding", while the 1 sσ potential well becomes deeper. For larger Z, the 1 sσ orbital eventually becomes "antibonding" but the potential curve passes through a number of distinct intermediate stages before a purely repulsive potential is reached.
| Original language | English |
|---|---|
| Pages (from-to) | 87-90 |
| Number of pages | 4 |
| Journal | Theoretica Chimica Acta |
| Volume | 12 |
| Issue number | 1 |
| DOIs | |
| State | Published - Jan 1968 |