Model for hypernucleus production in heavy ion collisions
arXiv:1002.4824 · doi:10.1103/PhysRevC.81.054911
Abstract
We estimate the production cross sections of hypernuclei in projectile like fragment (PLF) in heavy ion collisions. The discussed scenario for the formation cross section of hypernucleus is: (a) Lambda particles are produced in the participant region but have a considerable rapidity spread and (b) Lambda with rapidity close to that of the PLF and total momentum (in the rest system of PLF) up to Fermi motion can then be trapped and produce hypernuclei. The process (a) is considered here within Heavy Ion Jet Interacting Generator HIJING-BBbar model and the process (b) in the canonical thermodynamic model (CTM). We estimate the production cross-sections for light hypernuclei for C + C at 3.7 GeV total nucleon-nucleon center of mass energy and for Ne+Ne and Ar+Ar collisions at 5.0 GeV. By taking into account explicitly the impact parameter dependence of the colliding systems, it is found that the cross section is different from that predicted by the coalescence model and large discrepancy is obtained for 6_He and 9_Be hypernuclei.
9 pages, 4 figures, 3 tables, revtex4, added references
References in corpus (11)
- Thermal Dileptons at LHC
- Heavy-Quark Kinetics in the QGP at LHC
- Heavy Ion Collisions at the LHC - Last Call for Predictions
- Production of hypernuclei in multifragmentation of nuclear spectator matter
- Searching for onset of deconfinement via hypernuclei and baryon-strangeness correlations
- Formation of hypernuclei in high energy reactions within a covariant transport model
- Transient field fluctuations effects in d+Au and Au+Au collisions at \sqrt{s_nn} = 200 GeV
- Lambda hyperonic effect on the normal driplines
- Properties of the largest fragment in multifragmentation: a canonical thermodynamic calculation
- Extending the canonical thermodynamic model: inclusion of hypernuclei
- Soft Open Charm Production in Heavy-Ion Collisions
Cited by in corpus (20)
- Strangeness in nuclear physics
- Parton-Hadron-Quantum-Molecular Dynamics (PHQMD) -- A Novel Microscopic N-Body Transport Approach for Heavy-Ion Collisions, Dynamical Cluster Formation and Hypernuclei Production
- Formation of hypermatter and hypernuclei within transport models in relativistic ion collisions
- Light Neutron-Rich Hypernuclei from the Importance-Truncated No-Core Shell Model
- Production of spectator hypermatter in relativistic heavy-ion collisions
- Formation of hypernuclei in heavy-ion collisions around the threshold energies
- Production of antimatter Li nuclei in central Au+Au collisions at GeV
- Production of hypernuclei in peripheral relativistic ion collisions
- Centrality dependence of light (anti)nuclei and (anti)hypertriton production in Au+Au collisions at = 200 GeV
- Energy dependence of light (anti)nuclei and (anti)hypertriton production in the Au-Au collision from to GeV
- Antimatter production in central Au+Au collisions at =200 GeV
- Light anti-nuclei production in pp collisions at =7 and 14 TeV
- Estimates for temperature in projectile like fragment in geometric and transport models
- Scaling Properties of light (anti)nuclei and (anti)hypertriton production in Au+Au collisions at GeV
- Properties of light (anti)nuclei and (anti) hypertriton production in Pb-Pb collisions at = 2.76 TeV
- Predictions for production of and in isobaric Ru+Ru and Zr+Zr collisions at = 200 GeV
- Light (anti)nuclei production in Cu+Cu collisions at GeV
- Light (anti-)nuclei and (anti-)hypertriton production in collisions at and TeV
- Liquid gas phase transition in hypernuclei
- Effect of hyperons on phase coexistence in strange matter