Lepton flavor violating $μ\to eγ$ and $μ-e$ conversion in unparticle physics
| dc.creator | Ding, Gui-Jun | |
| dc.creator | Yan, Mu-Lin | |
| dc.date | 2007-09-21 | |
| dc.date | 2008-11-28 | |
| dc.date.accessioned | 2026-07-07T12:04:55Z | |
| dc.date.available | 2026-07-07T12:04:55Z | |
| dc.description | We have studied lepton flavor violation processes $μ\to eγ$ and $μ-e$ conversion in nuclei induced by unparticle. Both ${\rm Br}(μ\to eγ)$ and $μ-e$ conversion rate ${\rm CR}(μ-e,{\rm Nuclei})$ strongly depend on the scale dimension $d_{\cal U}$ and the unparticle coupling $λ^{ff'}_{\rm K}$(K=V, A, S, P). Present experimental upper bounds on ${\rm Br}(μ\to eγ)$, ${\rm CR}(μ-e,{\rm Ti})$ and ${\rm CR}(μ-e,{\rm Au})$ put stringent constraints on the parameters of unaprticle physics. The scale dimensions $d_{\cal U}$ around 2 are favored for the unparticle scale $Λ_{\cal U}$ of ${\cal O}(10 {\rm TeV})$ and the unparticle coupling of ${\cal O}(10^{-3})$. ${\rm CR}(μ-e,{\rm Nuclei})$ is proportional to $\rm{Z^4_{eff}A^2/Z}$ for the pure vector and scalar couplings between unparticle and SM fermions, this peculiar atomatic number dependence can be used to distinguish unparticle from other theoretical models. | |
| dc.description | 16 pages, 5 figures | |
| dc.identifier | https://arxiv.org/abs/0709.3435 | |
| dc.identifier | http://arxiv.org/abs/0709.3435 | |
| dc.identifier | Phys.Rev.D77:014005,2008 | |
| dc.identifier | doi:10.1103/PhysRevD.77.014005 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/208246 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Lepton flavor violating $μ\to eγ$ and $μ-e$ conversion in unparticle physics | |
| dc.type | text |