On the problem of unboundedness from below of the spinor QED Hamiltonian
| dc.creator | Zastavenko, L. G. | |
| dc.date | 1993-02-25 | |
| dc.date.accessioned | 2026-07-07T04:19:18Z | |
| dc.date.available | 2026-07-07T04:19:18Z | |
| dc.description | We show that the Hamiltonian $ h= H_{QED}+H_2$, where $H_{QED}$ is the spinor QED Hamiltonian and $H_2$ is the positive transversal photon mass term, is unbounded from below if the electromagnetic coupling constant $e^2$ is small enough, $e^2<e^2_0 $, and the transversal photon squared mass parameter $M^2$ is not too large: $0\leq M^2<e^2l^2c$, here, $l$ is the cut-off parameter, and $c$ and $e^2_0$, positive constants which do not depend on any parameters. | |
| dc.description | 14pages, latex | |
| dc.identifier | https://arxiv.org/abs/hep-th/9302128 | |
| dc.identifier | http://arxiv.org/abs/hep-th/9302128 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/53495 | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | On the problem of unboundedness from below of the spinor QED Hamiltonian | |
| dc.type | text |