dc.creator |
Adlarson, P. |
|
dc.creator |
Afzal, F. |
|
dc.creator |
Aguar-Bartolome, P. |
|
dc.creator |
Ahmed, Z. |
|
dc.creator |
Annand, J. R. M. |
|
dc.creator |
Arends, H. J. |
|
dc.creator |
Bantawa, K. |
|
dc.creator |
Beck, R. |
|
dc.creator |
Berghauser, H. |
|
dc.creator |
Biroth, M. |
|
dc.creator |
Borisov, N. S. |
|
dc.creator |
Braghieri, A. |
|
dc.creator |
Briscoe, W. J. |
|
dc.creator |
Cherepnya, S. |
|
dc.creator |
Cividini, F. |
|
dc.creator |
Collicott, C. |
|
dc.creator |
Costanza, S. |
|
dc.creator |
Danilkin, I. V. |
|
dc.creator |
Denig, A. |
|
dc.creator |
Dieterle, M. |
|
dc.creator |
Downie, E. J. |
|
dc.creator |
Drexler, P. |
|
dc.creator |
Ferretti-Bondy, M. I. |
|
dc.creator |
Fil’kov, L. V. |
|
dc.creator |
Gardner, S. |
|
dc.creator |
Garni, S. |
|
dc.creator |
Glazier, D. I. |
|
dc.creator |
Glowa, D. |
|
dc.creator |
Gradl, W. |
|
dc.date.accessioned |
2021-08-10T15:13:57Z |
|
dc.date.available |
2021-08-10T15:13:57Z |
|
dc.date.issued |
2017-03-22 |
|
dc.identifier.issn |
2469-9985 |
|
dc.identifier.uri |
http://library2.smu.ca/xmlui/handle/01/29731 |
|
dc.description |
Accepted Version |
en_CA |
dc.description.abstract |
The Dalitz decays η→e<sup>+</sup>e<sup>−</sup>γ and ω→π<sup>0</sup>e<sup>+</sup>e<sup>−</sup> have been measured in the γp→ηp and γp→ωp reactions, respectively, with the A2 tagged-photon facility at the Mainz Microtron. The value obtained for the slope parameter of the electromagnetic transition form factor of η, Λ<sup>−2</sup><sub>η</sub>=(1.97±0.11<sub>tot</sub>)GeV<sup>−2</sup>, is in good agreement with previous measurements of the η→e<sup>+</sup>e<sup>−</sup>γ and η→μ<sup>+</sup>μ<sup>−</sup>γ decays. The uncertainty obtained in the value of Λ<sup>−2</sup><sub>η</sub> is lower than in previous results based on the η→e<sup>+</sup>e<sup>−</sup>γ decay. The value obtained for the ω slope parameter, Λ<sup>−2</sup><sub>ωπ<sup>0</sup></sub>=(1.99±0.21<sub>tot</sub>)GeV<sup>−2</sup>, is somewhat lower than previous measurements based on ω→π<sup>0</sup>μ<sup>+</sup>μ<sup>−</sup>, but the results for the ω transition form factor are in better agreement with theoretical calculations, compared to earlier experiments. |
en_CA |
dc.description.provenance |
Submitted by Sherry Briere (sherry.briere@smu.ca) on 2021-08-10T15:13:57Z
No. of bitstreams: 1
Collicott_C_article_2017.pdf: 825602 bytes, checksum: 3b909f2774133225de88a0f16da79ebf (MD5) |
en |
dc.description.provenance |
Made available in DSpace on 2021-08-10T15:13:57Z (GMT). No. of bitstreams: 1
Collicott_C_article_2017.pdf: 825602 bytes, checksum: 3b909f2774133225de88a0f16da79ebf (MD5)
Previous issue date: 2017-03-22 |
en |
dc.language.iso |
en |
en_CA |
dc.publisher |
American Physical Society |
en_CA |
dc.relation.uri |
https://dx.doi.org/10.1103/PhysRevC.95.035208 |
|
dc.subject.lcsh |
Electromagnetism |
|
dc.subject.lcsh |
Microtrons |
|
dc.title |
Measurement of the ω→π0e+e− and η→e+e−γ Dalitz decays with the A2 setup at the Mainz Microtron |
en_CA |
dc.title.alternative |
Measurement of the omega -> pi[superscript 0]e[superscript +]e[superscript -] and eta -> e[superscript +]e[superscript -]gamma Dalitz decays with the A2 setup at the Mainz Microtron |
|
dc.type |
Text |
en_CA |
dcterms.bibliographicCitation |
Physical Review C 95(3), 035208. (2017) |
en_CA |