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dc.date.accessioned |
2014-03-01T01:43:36Z |
|
dc.date.available |
2014-03-01T01:43:36Z |
|
dc.date.issued |
1995 |
en |
dc.identifier.issn |
01709739 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/24165 |
|
dc.title |
B* production in Z decays |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1007/BF01620711 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1007/BF01620711 |
en |
heal.publicationDate |
1995 |
en |
heal.abstract |
The decay B*→Bγ has been observed with the DELPHI detector at LEP, where the B* meson is produced in Z boson decays. The combination of inclusively reconstructed B mesons with well-measured converted photons yields a measurement of the flavour-averaged B*-B mass difference of 45.5±0.3 (stat.) ±0.8 (syst.) MeV/c2. 95% confidence level upper limits at 6 MeV/c2 are placed on both the isospin (i.e. B+-B0) and the Bs-Bud splitting of the mass difference. The production ratio of B* to B mesons in Z decays is measured to be 0.72±0.03 (stat.) ±0.06 (syst.). Limits on the production cross-section of other hypothetical excited B hadron states decaying radiatively are established. The differential B* cross section has been measured to be in good agreement with the average b fragmentation, yielding an average fractional B* energy of 〈xE〉=0.695±0.009 (stat.) ±0.013 (syst.). From the decay angular distribution the relative contribution of longitudinal B* polarisation states is measured to be σL/(σL + σT) = 0.32 ± 0.04 (stat.) ±0.03 (syst.). © 1995 Springer-Verlag. |
en |
heal.publisher |
Springer-Verlag |
en |
heal.journalName |
Zeitschrift für Physik C Particles and Fields |
en |
dc.identifier.doi |
10.1007/BF01620711 |
en |
dc.identifier.volume |
68 |
en |
dc.identifier.issue |
3 |
en |
dc.identifier.spage |
353 |
en |
dc.identifier.epage |
362 |
en |