Preferred basis without decoherence
| dc.creator | Vanni, L. | |
| dc.creator | Laura, R. | |
| dc.date | 2008-11-29 | |
| dc.date | 2008-12-02 | |
| dc.date.accessioned | 2026-07-07T12:08:09Z | |
| dc.date.available | 2026-07-07T12:08:09Z | |
| dc.description | The aim of this paper is to argue that the "preferred basis problem" is not a real problem in measurement. We will show that, given an apparatus, among the infinite corrrelations that can be established in the final state by means of a change of basis, one and only one makes physical sense. It is the apparatus, through its interaction Hamiltonian, what selects a single basis and determines the observable to be measured, even without decoherence. | |
| dc.description | 11 pages | |
| dc.identifier | https://arxiv.org/abs/0812.0093 | |
| dc.identifier | http://arxiv.org/abs/0812.0093 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/209217 | |
| dc.subject | Quantum Physics | |
| dc.title | Preferred basis without decoherence | |
| dc.type | text |