Qubit Field Theory
| dc.creator | Deutsch, David | |
| dc.date | 2004-01-06 | |
| dc.date.accessioned | 2026-07-07T06:08:44Z | |
| dc.date.available | 2026-07-07T06:08:44Z | |
| dc.description | The canonical commutation relations of quantum field theory require all pairs of observables located in spacelike-separated regions to commute. In the theory as it is currently constituted, this implies that the information-carrying capacity of a finite volume of space is infinite. Yet Bekenstein's bound gives us strong reason to believe that it is finite. A class of quantum field theories is presented in which observables localised in spacelike-separated regions do not necessarily commute, but which nevertheless has no physical pathologies. | |
| dc.identifier | https://arxiv.org/abs/quant-ph/0401024 | |
| dc.identifier | http://arxiv.org/abs/quant-ph/0401024 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/91735 | |
| dc.subject | Quantum Physics | |
| dc.title | Qubit Field Theory | |
| dc.type | text |