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2015 ◽  
Vol 24 (07) ◽  
pp. 1550050 ◽  
Author(s):  
E. Matsinos ◽  
G. Rasche

In a previous paper, we reported the results of a partial-wave analysis (PWA) of the pion–nucleon (πN) differential cross-sections (DCSs) of the CHAOS Collaboration and came to the conclusion that the angular distribution of their π+p data sets is incompatible with the rest of the modern (meson factory) database. The present work, re-addressing this issue, has been instigated by a number of recent improvements in our analysis, namely regarding the inclusion of the theoretical uncertainties when investigating the reproduction of experimental data sets on the basis of a given "theoretical" solution, modifications in the parametrization of the form factors of the proton and of the pion entering the electromagnetic part of the πN amplitude, and the inclusion of the effects of the variation of the σ-meson mass when fitting the ETH model of the πN interaction to the experimental data. The new analysis of the CHAOS DCSs confirms our earlier conclusions and casts doubt on the value for the πN Σ term, which Stahov, Clement and Wagner have extracted from these data.



2012 ◽  
Vol 83 (2) ◽  
pp. 02A914 ◽  
Author(s):  
P. G. Bricault ◽  
F. Ames ◽  
M. Dombsky ◽  
F. Labrecque ◽  
J. Lassen ◽  
...  


2010 ◽  
Vol 52 (5) ◽  
pp. 1021-1024 ◽  
Author(s):  
Yu. V. Ryabov ◽  
M. I. Grachev ◽  
D. V. Kamanin ◽  
E. A. Kuznetsova ◽  
V. L. Kuznetsov ◽  
...  


2009 ◽  
Vol 52 (6) ◽  
pp. 769-773 ◽  
Author(s):  
Yu. M. Burmistrov ◽  
S. V. Zuyev ◽  
E. S. Konobeevski ◽  
M. V. Mordovskoy ◽  
S. I. Potashev ◽  
...  


2005 ◽  
Vol 20 (15) ◽  
pp. 3531-3534
Author(s):  
◽  
PAUL E. KUTTER

We present results on time-dependent CP asymmetries in [Formula: see text] and B0 → K+K-K0. The measurements use a data sample consisting of approximately [Formula: see text] and 227(B0 → K+K-K0) million B-meson pairs recorded at the ϒ(4S) resonance with the BABAR detector at the PEP-II B-meson Factory at SLAC. From a time-dependent maximum likelihood fit, we measure for [Formula: see text]: the mixing-induced CP violation parameter [Formula: see text] and the direct CP violation parameter Cf0K = -0.24 ± 0.31 ( stat ) ± 0.15 ( syst ). From a simultaneous fit to [Formula: see text] and [Formula: see text] decays, we find: [Formula: see text] and CϕK = 0.00 ± 0.23 ( stat ) ± 0.05 ( syst ). For [Formula: see text] decays with [Formula: see text] decays excluded, we find: [Formula: see text] and [Formula: see text]. From the [Formula: see text] decays with [Formula: see text] decays excluded, we extract the fraction of CP-even final states from angular moments feven = 0.89 ± 0.08 ± 0.06.





Author(s):  
A. Garren ◽  
S. Chattopadhyay ◽  
Y. Chin ◽  
P. Oddone ◽  
M.S. Zisman ◽  
...  
Keyword(s):  
B Meson ◽  


Author(s):  
V.A. Andreev ◽  
V.A. Bomko ◽  
G.N. Vjalov ◽  
S.K. Esin ◽  
D.V. Gorelov ◽  
...  


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