Measurement of radiative widths of $a_2(1320)$ and $Ï_2(1670)$
arXiv:1403.2644 · doi:10.1140/epja/i2014-14079-8
Abstract
The COMPASS Collaboration at CERN has investigated the reaction $Ï^- γ\rightarrow Ï^-Ï^-Ï^+$ embedded in the Primakoff reaction of $190~\textrm{GeV}$ pions scattering in the Coulomb field of a lead target, $Ï^- \text{Pb} \rightarrow Ï^-Ï^-Ï^+ \text{Pb}$. Exchange of quasi-real photons is selected by isolating the sharp Coulomb peak observed at momentum transfer below $0.001~(\text{GeV}/c)^2$. Using a partial-wave analysis the amplitudes and relative phases of the $a_2(1320)$ and $Ï_2(1670)$ mesons have been extracted, and the Coulomb and the diffractive contributions have been disentangled. Measuring absolute production cross sections we have determined the radiative width of the $a_2(1320)$ to be $Î_0(a_2(1320) \rightarrow Ïγ) = (358 \pm 6_{\textrm{stat}} \pm 42_{\textrm{syst}})~\textrm{keV}$. As the first measurement, $Î_0(Ï_2(1670) \rightarrow Ïγ) = (181 \pm 11_{\textrm{stat}} \pm 27_{\textrm{syst}})~\textrm{keV} \cdot (\textrm{BR}^{\textrm{PDG}}_{f_2 Ï}/\textrm{BR}_{f_2 Ï})$ is obtained for the radiative width of the $Ï_2(1670)$, where in this analysis the branching ratio $\textrm{BR}^{\textrm{PDG}}_{f_2 Ï}=0.56$ has been used. We compare these values to previous measurements and theoretical predictions.
27 pages, 12 figures and 3 tables