Three-Body Hypernuclei in Pionless Effective Field Theory
arXiv:1904.05818 · doi:10.1103/PhysRevC.100.034002
Abstract
We calculate the structure of three-body hypernuclei with using pionless effective field theory at leading order in the isospin and sectors. In both sectors, three-body hypernuclei arise naturally from the Efimov effect and a three-body parameter is required at leading order. We apply our theory to the hypertriton and the hypothetical bound state and calculate the corresponding scaling factors. Moreover, we discuss constraints on the existence of the bound state. In particular, we elucidate universal correlations between different observables and provide explicit calculations of wave functions and matter radii.
26 pages, 13 figures, typos corrected, discussion of parameter space for Lambda_* extended, error in Figs. 5-7 and Lambda-d scattering length corrected, final version
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- Towards the understanding of the genuine three-body interaction for ppp and pp
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- Nature of the and states
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- Deuteron yields from LHC: Continuum correlations and in-medium effects
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- Probing the size and binding energy of the hypertriton in heavy ion collisions
- First measurement of A = 4 (anti)hypernuclei at the LHC
- Consequences of increased hypertriton binding for -shell -hypernuclear systems
- Measurement of production in Pb-Pb collisions at = 5.02 TeV
- Faddeev calculations of low-energy -deuteron scattering and momentum correlation function
- Study on Bound State and Resonance
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- H and He Hypernuclei reexamined in Halo/Cluster Effective Theory
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- A Data-Guided Coalescence Model for Light Nuclei and Hypernuclei Production in Relativistic Heavy-Ion Collisions at --200 GeV