Parity non-conservation in thallium
| dc.creator | Kozlov, M G | |
| dc.creator | Porsev, S G | |
| dc.creator | Johnson, W R | |
| dc.date | 2001-05-27 | |
| dc.date.accessioned | 2026-07-07T05:45:52Z | |
| dc.date.available | 2026-07-07T05:45:52Z | |
| dc.description | We report a new calculation of the parity non-conserving E1 amplitude for the 6p_{1/2} -> 6p_{3/2} transition in Tl. Our result for the reduced matrix element is $E1_{PNC}=-(66.7 \pm 1.7) i 10^{-11} (-Q_W/N)$ a.u. Comparison with the experiment of Vetter et al [PRL,{\bf 74},2658 (1995)] gives the following result for the weak charge of $^{205}$Tl: $Q_W/Q_W^{SM} = 0.97 (\pm 0.01)_{expt} (\pm 0.03)_{theor}$, where $Q_W^{SM}=-116.7$ is the standard model prediction. This result confirms an earlier conclusion based on the analysis of a Cs experiment that atomic PNC experiments are in agreement with the standard model. | |
| dc.description | 6 pages, LaTeX2e, uses revtex4.cls, submitted to PRA | |
| dc.identifier | https://arxiv.org/abs/physics/0105090 | |
| dc.identifier | http://arxiv.org/abs/physics/0105090 | |
| dc.identifier | PRA, 64, 052107 (2001) | |
| dc.identifier | doi:10.1103/PhysRevA.64.052107 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/84146 | |
| dc.subject | Atomic Physics | |
| dc.title | Parity non-conservation in thallium | |
| dc.type | text |