The heavy tetra-quark states after the discovery of tetra-charm states
arXiv:2204.10721 · doi:10.1140/epjc/s10052-022-10924-7
Abstract
This paper is devoted to the study of exclusive charm and bottom aggregates which are suitable, at least partially, for a non-relativistic description. Starting from a simple choice of quarkonia and tetra-quark wave functions we study their production cross sections, total widths and more interesting decay properties. In particular, we compute the production cross sections of the ground state scalar quarkonia getting results compatible with the values appearing in the literature. We also compute the production cross sections of the lower energy states of the charm and bottom tetra-quarks, their decay widths and the decay rates in two pairs and in the channel. Our results on the tetra-charm are consistent with the data published by the LHCb Collaboration and those on the tetra-bottom show a reasonable agreement with the indications published by the CMS Collaboration. Our cross section analyses are based on interpolations based on the gluon-gluon luminosity grids published by the NNPDF and CTEQ Collaborations. The hard amplitude calculations are based on QCD in the tree approximation. We think that a careful improvement of our method and a refinement of the experimental data after the foreseen luminosity increase at the LHC will make possible valuable tests of QCD at the intermediate energies.
33 pages, 21 figures
References in corpus (9)
- Parton distributions for the LHC
- New parton distributions for collider physics
- Observation of structure in the -pair mass spectrum
- Hard Interactions of Quarks and Gluons: a Primer for LHC Physics
- A study of tetraquark decays in 4 muons and in at LHC
- Search for tetraquark decays in 4 muons, , and channels at LHC
- Nonrelativistic model of tetraquarks and predictions for their masses from fits to charmed and bottom meson data
- Exotic resonances of fully-heavy tetraquarks in a lattice-QCD insipired quark model
- Bottomonium spectrum with a Dirac potential model in the momentum space