Light nuclei and hypernuclei from quantum chromodynamics in the limit of SU(3) flavor symmetry
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Abstract
The binding energies of a range of nuclei and hypernuclei with atomic number $A\ensuremath{\le}4$ and strangeness $|s|\ensuremath{\le}2$, including the deuteron, dineutron, H-dibaryon, $^{3}\mathrm{He}$, $_{\ensuremath{\Lambda}}^{3}\mathrm{He}$, $^{4}\mathrm{He}$, $_{\ensuremath{\Lambda}}^{4}\mathrm{He}$, and $_{\ensuremath{\Lambda}\ensuremath{\Lambda}}^{4}\mathrm{He}$, are calculated in the limit of flavor-SU(3) symmetry at the physical strange-quark mass with quantum chromodynamics (without electromagnetic interactions). The nuclear states are extracted from lattice QCD calculations performed with ${n}_{f}=3$ dynamical light quarks using an isotropic clover discretization of the quark action in three lattice volumes of spatial extent $L\ensuremath{\sim}3.4\text{ }\text{ }\mathrm{fm}$, 4.5 fm, and 6.7 fm, and with a single lattice spacing $b\ensuremath{\sim}0.145\text{ }\text{ }\mathrm{fm}$.
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