no code implementations • 2 Jun 2020 • Waleed Abdallah, Raj Gandhi, Samiran Roy
Choosing benchmark parameter values, we show that $U(1)_{B-3L_\tau}$, which is anomaly-free, and $U(1)_B$, both provide (phenomenologically) equally good solutions to the excess.
High Energy Physics - Phenomenology High Energy Physics - Experiment
