Production of hypernuclei in relativistic ion beams
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Cited by (23)
Hypernuclear production cross section in the reaction of <sup>6</sup>Li + <sup>12</sup>C at 2A GeV
2015, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsCitation Excerpt :Yet the extremely scarce experimental data currently available do not restrain those models. One has to also notice that first theoretical work from [8,12–14] and updated calculations [22–24] differ by order of magnitude on the prediction of the hypernuclear production cross sections. Recently, the HypHI Collaboration has observed the production of light hypernuclei, 3ΛH and 4ΛH in a reaction with 6Li projectiles impinging on a graphite (natC) target [25].
Formation of hypernuclei in high energy reactions within a covariant transport model
2009, Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy PhysicsCitation Excerpt :However, the life time of hypernuclei seen in the laboratory is considerably enhanced in relativistic collisions due to relativistic effects. Hypernuclear production in proton-induced reactions has been experimentally studied also at COSY [9] and the comparison with theoretical predictions based on transport equations of the Boltzmann type has been successfully performed [10]. More recently, concrete experimental proposals with high energy heavy-ion and proton beams at GSI (Darmstadt, Germany) and J-PARC (Japan), respectively, have been suggested by Saito [11,12].
Production of fragments with and without strangeness within a combined BUU + SMM approach
2009, Progress in Particle and Nuclear PhysicsCitation Excerpt :The theoretical production of light hypernuclei in reactions was originally proposed by Kerman and Weiss [2]. Since then this topic has been attracted again theoretical interest [3], motivated by the new FAIR facility at GSI, in which projects on hypernuclear physics are running or under planning [4,5]. In this work the initial non-equilibrium stage of a reaction is described by a covariant transport theory of Boltzmann type (Giessen-BUU), while the fragmentation mechanism of the final channel is modeled by a purely statistical approach (Statistical Multifragmentation Model, SMM [6]).
Energy levels of light nuclei, A = 20
1998, Nuclear Physics AEnergy levels of light nuclei A = 18-19
1995, Nuclear Physics, Section AHypernuclear structure
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