Such a flavourless meson, also called a χ (chi) particle, exists at various excited states, or excitation modes, just like a hydrogen atom, and it decays to each state by the radiation of a photon (γ). The Upsilon meson was first observed in 1977 in an experiment headed by Leon Lederman at the Fermilab, Chicago, with a mass of 9.46 GeV/c2. The ATLAS discovery corresponds to a higher excitation state, χb (3P), wherein the particle's mass is 10.539 ± 0.004 GeV/c2.
[caption id="attachment_21088" align="aligncenter" width="600" caption="The spike in activity corresponds to a detection. The Upsilon meson was observed in three independent channels."]
Like the electronic orbitals in an atom, each decay state is designated as belonging to an S, P or D energy-state, and the discovery is that of a χb (3P): a flavourless meson at the 3P excitation mode. In the second diagram, the particle shows up as the right-most peak on the purple (lowermost) curve, corresponding to ~10.5 GeV on the x-axis. It hasn't shown up in earlier experiments because only the Large Hadron Collider has been able to supply the high rate of collisions required to record the particle's existence before it decays in 1.21×10−20 seconds (at 9.46 GeV/c2).
The corresponding pre-print paper submitted by the ATLAS Collaboration is available here.
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