Unparticle as a field with continuously distributed mass
| dc.creator | Krasnikov, N. V. | |
| dc.date | 2007-07-10 | |
| dc.date | 2007-08-08 | |
| dc.date.accessioned | 2026-07-07T11:17:41Z | |
| dc.date.available | 2026-07-07T11:17:41Z | |
| dc.description | We point out that the notion of an unparticle, recently introduced by Georgi, can be interpreted as a particular case of a field with continuously distributed mass considered in ref.\cite{14}. We also point out that the simplest renormalizable extension of the $SU_c(3)\otimes SU_L(2)\otimes U(1)$ Standard Model is the extension with the replacement of the U(1) gauge propagator $\frac{1}{k^2} \to \frac{1}{k^2} + \int _0^{\infty}\frac{ρ(t)}{-t+k^2 +iε}dt$ with $\int_0^{\infty}ρ(t)dt < \infty $. | |
| dc.description | 6 pages, added references, corrected typos | |
| dc.identifier | https://arxiv.org/abs/0707.1419 | |
| dc.identifier | http://arxiv.org/abs/0707.1419 | |
| dc.identifier | Int.J.Mod.Phys.A22:5117-5120,2007 | |
| dc.identifier | doi:10.1142/S0217751X07037342 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/193090 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Unparticle as a field with continuously distributed mass | |
| dc.type | text |