The decay asymmetries of the weak radiative hyperon decays Xi0 -> Lambda gamma and Xi0 -> Sigma0 gamma have been measured with high precision using data of the NA48/1 experiment at CERN. From about 52 000 Xi0 -> Lambda gamma and 15 000 Xi0 -> Sigma0 gamma decays, we obtain for the decay asymmetries alpha(Xi0 -> Lambda gamma) = -0.704 +-0.019stat +-0.064syst and alpha(Xi0 -> Sigma0 gamma) = -0.729 +-0.030stat +-0.076syst , respectively. These results are in good agreement with previous experiments, but more precise.
New precise measurements of the Ξ0→Λγ and Ξ0→Σ0γ decay asymmetries / J. R., B., G. E., K., C., L., D. J., M., M., P., M. W., S., S. A., W., R., A., G., B., A., C., D., C., N., D., V., F., L., G., A., G., P., G., W., K., I., M., A., N., B., P.S., et al.. - In: PHYSICS LETTERS. SECTION B. - ISSN 0370-2693. - STAMPA. - 693:3(2010), pp. 241-248. [10.1016/j.physletb.2010.08.046]
New precise measurements of the Ξ0→Λγ and Ξ0→Σ0γ decay asymmetries
BIZZETI, Andrea;
2010
Abstract
The decay asymmetries of the weak radiative hyperon decays Xi0 -> Lambda gamma and Xi0 -> Sigma0 gamma have been measured with high precision using data of the NA48/1 experiment at CERN. From about 52 000 Xi0 -> Lambda gamma and 15 000 Xi0 -> Sigma0 gamma decays, we obtain for the decay asymmetries alpha(Xi0 -> Lambda gamma) = -0.704 +-0.019stat +-0.064syst and alpha(Xi0 -> Sigma0 gamma) = -0.729 +-0.030stat +-0.076syst , respectively. These results are in good agreement with previous experiments, but more precise.| File | Dimensione | Formato | |
|---|---|---|---|
|
1009.3844.pdf
Open access
Tipologia:
VOR - Versione pubblicata dall'editore
Dimensione
246.82 kB
Formato
Adobe PDF
|
246.82 kB | Adobe PDF | Visualizza/Apri |
Pubblicazioni consigliate

I metadati presenti in IRIS UNIMORE sono rilasciati con licenza Creative Commons CC0 1.0 Universal, mentre i file delle pubblicazioni sono rilasciati con licenza Attribuzione 4.0 Internazionale (CC BY 4.0), salvo diversa indicazione.
In caso di violazione di copyright, contattare Supporto Iris




