Hyperfine splittings in the system
arXiv:0912.2259 · doi:10.1016/j.nuclphysa.2011.06.032
Abstract
Recent measurements of the , the ground state of the system, show the splitting between it and the $\Up(1S)$ to be 69.53.2 MeV, considerably larger than lattice QCD and potential model predictions, including recent calculations published by us. The models are unable to incorporate such a large hyperfine splitting within the context of a consistent description of the energy spectrum and decays. We demonstrate that in our model, which incorporates a relativistic kinetic energy term, a linear confining term including its scalar-exchange relativistic corrections, and the complete one-loop QCD short distance potential, such a consistent description, including the measured hyperfine splitting, can be obtained by not softening the delta function terms in the hyperfine potential. We calculate the hyperfine splitting to be 67.5 MeV.
5 pages, 3 tables, text revisions
References in corpus (7)
- Potential model calculations and predictions for heavy quarkonium
- Quarkonium mass splittings in three-flavor lattice QCD
- Bottomonium spectrum at order v^6 from domain-wall lattice QCD: precise results for hyperfine splittings
- Measurement of the eta_b(1S) mass and the branching fraction for Upsilon(3S) --> gamma eta_b(1S)
- Bottomonium spectroscopy with mixing of eta_b states and a light CP-odd Higgs
- The bottomonium spectrum from lattice QCD with 2+1 flavors of domain wall fermions
- The Hyperfine Splittings in Bottomonium and the Mesons
Cited by in corpus (12)
- Higher mass bottomonia
- () spectroscopy using Cornell potential
- Leptonic and Digamma decay Properties of S-wave quarkonia states
- Status of quarkonia - like negative and positive parity states in a relativistic confinement scheme
- meson spectroscopy motivated by general features of pNRQCD
- Chi_b(3P) splitting predictions in potential models
- Hyperfine splitting and the experimental candidates for η_b(2S)
- Bottomonium spectroscopy motivated by general features of pNRQCD
- Unified covariant treatment of hyperfine splitting for heavy and light mesons
- Relativistic two fermion treatment of hyperfine transitions
- Relativistic two-body calculation of -mesons radiative decays
- Spin splitting spectroscopy of heavy quark anti quark systems