Observation of eta_b(2S) in Upsilon(2S) -> gamma eta_b(2S), eta_b(2S) -> hadrons, and Confirmation of eta_b(1S)
arXiv:1204.4205 · doi:10.1103/PhysRevLett.109.082001
Abstract
The data for 9.3 million Upsilon(2S) and 20.9 million Upsilon(1S) taken with the CLEO III detector has been used to study the radiative population of states identified by their decay into twenty six different exclusive hadronic final states. In the Upsilon(2S) decays an enhancement is observed at a ~5 sigma level at a mass of 9974.6+-2.3(stat)+-2.1(syst) MeV. It is attributed to eta_b(2S), and corresponds to the Upsilon(2S) hyperfine splitting of 48.7+-2.3(stat)+-2.1(syst) MeV. In the Upsilon(1S) decays, the identification of eta_b(1S) is confirmed at a ~3 sigma level with M(eta_b(1S)) in agreement with its known value.
5 pages, 2 figures
References in corpus (2)
Cited by in corpus (21)
- QCD and strongly coupled gauge theories: challenges and perspectives
- Bottomonium spectrum revisited
- Higher bottomonium zoo
- Improved determination of Heavy Quarkonium magnetic dipole transitions in pNRQCD
- Bottomonium spectrum in the relativistic flux tube model
- Recent Results in Bottomonium
- Bottomonium hyperfine splittings from lattice NRQCD including radiative and relativistic corrections
- Instanton effects on the heavy-quark static potential
- Hyperfine splitting and the experimental candidates for η_b(2S)
- Bottomonium spectroscopy motivated by general features of pNRQCD
- Search for Bottomonium States in Exclusive Radiative Upsilon(2S) Decays
- More about excited bottomonium radiative decays
- Bottomonium spectrum with a Dirac potential model in the momentum space
- Coulomb Artifacts and Bottomonium Hyperfine Splitting in Lattice NRQCD
- Bottomonium Hyperfine Splitting on the Lattice and in the Continuum
- An introduction to the quark model
- Observation of decay
- Predictions for Bottomonium from a Relativistic Screened Potential Model
- Relativistic two-body calculation of -mesons radiative decays
- Experimental review of the physics at colliders and the LHC
- Beauty Hadron Spectrum in a Screened Potential Model