Bottomonium Mesons and Strategies for Their Observation

preprint2015arXivOpen access

Abstract

The BB-factories and Large Hadron Collider experiments have demonstrated the ability to observe and measure the properties of bottomonium mesons. In order to discover missing states it is useful to know their properties to develop a successful search strategy. To this end we calculate the masses and decay properties of excited bottomonium states. We use the relativized quark model to calculate the masses and wavefunctions and the 3P0^3P_0 quark-pair creation model to calculate decay widths to open bottom. We also summarize results for radiative transitions, annihilation decays, hadronic transitions and production cross sections which are used to develop strategies to find these states. We find that the bbˉb\bar{b} system has a rich spectroscopy that we expect to be substantially extended by the LHC and e+e−e^+e^- experiments in the near future. Some of the most promising possibilities at the LHC are observing the χb(1,2)(3P)χ_{b(1,2)}(3P), χb(1,2)(4P)χ_{b(1,2)}(4P) and ηb(3S)η_b(3S) states in γμ+μ−γμ^+μ^- final states that proceed via radiative transitions through Υ(nS)Υ(nS) intermediate states and 13DJ1^3D_J and 23DJ2^3D_J into γγμ+μ−γγμ^+μ^- final states proceeding via 13PJ→13S11^3P_J\to 1^3S_1 and 23PJ→23S12^3P_J\to 2^3S_1 intermediate states respectively. Some of the most interesting possibilities in e+e−e^+e^- collisions are studying the 13DJ1^3D_J states via 4γ4γ cascades starting with the Υ(3S)Υ(3S) and the 33PJ3^3P_J states in γγμ+μ−γγμ^+ μ^- final states starting with the Υ(4S)Υ(4S) and proceeding via Υ(nS)Υ(nS) intermediate states. Completing the bottomonium spectrum is an important validation of lattice QCD calculations and a test of our understanding of bottomonium states in the context of the quark model.

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