Abstract
In π systems with localized double bonds, the switch from one localization pattern to another symmetry‐equivalent one, and the corresponding changes in electron distribution are often considered to proceed via a delocalized transition state of higher symmetry. We present a different mechanism, according to which the double‐bond localization and the concomitant charge distributions can fluctuate without change in energy and without passing through a delocalized, higher‐symmetry transition state. This result is obtained within a simple, independent‐electron (HMO‐type) treatment.
| Original language | English |
|---|---|
| Pages (from-to) | 539-556 |
| Number of pages | 18 |
| Journal | Helvetica Chimica Acta |
| Volume | 75 |
| Issue number | 2 |
| DOIs | |
| State | Published - 18 Mar 1992 |
| Externally published | Yes |
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