Abstract
We investigate the decays of the excited mesons as probes of the short-distance structure of the weak transitions. These states are unstable under the electromagnetic or strong interactions, although their widths are typically suppressed by phase space. Compared to the pseudoscalar meson, the purely leptonic decays of the vector are not chirally suppressed and are sensitive to different combinations of the underlying weak effective operators. An interesting example is , which has a rate that can be accurately predicted in the standard model. The branching fraction is , irrespective of the lepton flavor and where the main uncertainty stems from the unmeasured and theoretically not well known width. We discuss the prospects for producing this decay mode at the LHC and explore the possibility of measuring the amplitude, instead, through scattering experiments at the resonance peak.
- Received 28 October 2015
DOI:https://doi.org/10.1103/PhysRevLett.116.141801
© 2016 American Physical Society