Space/time noncommutative field theories and causality
| dc.creator | Bozkaya, H. | |
| dc.creator | Fischer, P. | |
| dc.creator | Grosse, H. | |
| dc.creator | Pitschmann, M. | |
| dc.creator | Putz, V. | |
| dc.creator | Schweda, M. | |
| dc.creator | Wulkenhaar, R. | |
| dc.date | 2002-09-30 | |
| dc.date | 2003-03-18 | |
| dc.date.accessioned | 2026-07-07T12:26:43Z | |
| dc.date.available | 2026-07-07T12:26:43Z | |
| dc.description | As argued previously, amplitudes of quantum field theories on noncommutative space and time cannot be computed using naive path integral Feynman rules. One of the proposals is to use the Gell-Mann--Low formula with time-ordering applied before performing the integrations. We point out that the previously given prescription should rather be regarded as an interaction point time-ordering. Causality is explicitly violated inside the region of interaction. It is nevertheless a consistent procedure, which seems to be related to the interaction picture of quantum mechanics. In this framework we compute the one-loop self-energy for a space/time noncommutative ϕ^4 theory. Although in all intermediate steps only three-momenta play a role, the final result is manifestly Lorentz covariant and agrees with the naive calculation. Deriving the Feynman rules for general graphs, we show, however, that such a picture holds for tadpole lines only. | |
| dc.description | 16 pages, LaTeX, uses feynmf macros, one reference added; ooops, version 2 was an older one! | |
| dc.identifier | https://arxiv.org/abs/hep-th/0209253 | |
| dc.identifier | http://arxiv.org/abs/hep-th/0209253 | |
| dc.identifier | Eur.Phys.J.C29:133-141,2003 | |
| dc.identifier | doi:10.1140/epjc/s2003-01210-9 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/214973 | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | Space/time noncommutative field theories and causality | |
| dc.type | text |