The binding energies of a range of nuclei and hypernuclei with atomic number A \u3c = 4 and strangeness vertical bar s vertical bar \u3c = 2, including the deuteron, dineutron, H - dibaryon, He - 3, He - 3 (Lambda), He - 4, He - 4(Lambda), and He - 4(Lambda Lambda), 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 similar to 3.4 fm, 4.5 fm, and 6.7 fm, and with a single lattice spacing b similar to 0.145 fm. DOI: 10.110...
The energy levels of light hypernuclei are experimentally accessible observables that contain valuab...
We calculate saturation curves for strange hadron matter using recently constructed baryon-baryon po...
Lattice quantum chromodynamics is used to constrain the interactions of two octet baryons at the SU(...
The binding energies of a range of nuclei and hypernuclei with atomic number A \u3c = 4 and strangen...
The binding energies of a range of nuclei and hypernuclei with atomic number A \u3c = 4 and strangen...
The binding energies of a range of nuclei and hypernuclei with atomic number A \u3c = 4 and strangen...
The binding energies of a range of nuclei and hypernuclei with atomic number A ≤ 4 and strangeness |...
The binding energies of a range of nuclei and hypernuclei with atomic number A ≤ 4 and strangeness |...
The low-energy n Σ − interactions determine, in part, the role of the strange quark in dense matter,...
Nucleon-nucleon systems are studied with lattice quantum chromodynamics at a pion mass of m(pi) simi...
The scattering lengths and effective ranges that describe low-energy nucleon-nucleon scattering are ...
Nucleon-nucleon systems are studied with lattice quantum chromodynamics at a pion mass of m(pi) simi...
The energy levels of light hypernuclei are experimentally accessible observables that contain valuab...
Quarkonium-nucleus systems are composed of two interacting hadronic states without common valence qu...
Quarkonium-nucleus systems are composed of two interacting hadronic states without common valence qu...
The energy levels of light hypernuclei are experimentally accessible observables that contain valuab...
We calculate saturation curves for strange hadron matter using recently constructed baryon-baryon po...
Lattice quantum chromodynamics is used to constrain the interactions of two octet baryons at the SU(...
The binding energies of a range of nuclei and hypernuclei with atomic number A \u3c = 4 and strangen...
The binding energies of a range of nuclei and hypernuclei with atomic number A \u3c = 4 and strangen...
The binding energies of a range of nuclei and hypernuclei with atomic number A \u3c = 4 and strangen...
The binding energies of a range of nuclei and hypernuclei with atomic number A ≤ 4 and strangeness |...
The binding energies of a range of nuclei and hypernuclei with atomic number A ≤ 4 and strangeness |...
The low-energy n Σ − interactions determine, in part, the role of the strange quark in dense matter,...
Nucleon-nucleon systems are studied with lattice quantum chromodynamics at a pion mass of m(pi) simi...
The scattering lengths and effective ranges that describe low-energy nucleon-nucleon scattering are ...
Nucleon-nucleon systems are studied with lattice quantum chromodynamics at a pion mass of m(pi) simi...
The energy levels of light hypernuclei are experimentally accessible observables that contain valuab...
Quarkonium-nucleus systems are composed of two interacting hadronic states without common valence qu...
Quarkonium-nucleus systems are composed of two interacting hadronic states without common valence qu...
The energy levels of light hypernuclei are experimentally accessible observables that contain valuab...
We calculate saturation curves for strange hadron matter using recently constructed baryon-baryon po...
Lattice quantum chromodynamics is used to constrain the interactions of two octet baryons at the SU(...