Triangle Singularity in the Production of (3875) and a Soft Pion
arXiv:2202.03900 · doi:10.1103/PhysRevD.106.034033
Abstract
The double-charm tetraquark meson can be produced in high-energy proton-proton collisions by the creation of the charm mesons at short distances followed by their binding into . The can also be produced by the creation of at short distances followed by their rescattering into . A charm-meson triangle singularity produces a narrow peak in the invariant mass distribution 6.1 MeV above the threshold with a width of about 1 MeV. Well beyond the peak, the differential cross section decreases with the invariant kinetic energy of as . The fraction of that are accompanied by with is estimated to be roughly 3%. The fraction of events with in the narrow peak from the triangle singularity could be comparable.
44 pages, 13 figures
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- Doubly-Charged States in the Dynamical Diquark Model
- Electromagnetic properties of the molecular states
- Triangle singularity in via the loop and possible precise measurement of the mass
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- Investigation on the bottom analogs of the
- Model-independent predictions for decays of double-heavy hadrons into pairs of heavy hadrons
- An alternative way to decipher the nature of the doubly charmed tetraquark : its antiparticle photoproduction off nuclei near threshold