In this review, we present the current state of the art of our understanding of the spectrum of
excited strongly interacting particles and discuss methods that allow for a systematic and …

We review the present status of the experimental and theoretical developments in the field of
strangeness in nuclei and neutron stars. We start by discussing the K ̄ N interaction, that is …

Extensions of nuclear physics to the strange sector are reviewed, covering data and models
of Λ and other hypernuclei, multistrange matter, and antikaon bound states and …

Abstract The S-wave ΛΛ and N Ξ interactions are studied on the basis of the (2+ 1)-flavor
lattice QCD simulations close to the physical point (m π≃ 146 MeV and m K≃ 525 MeV) …

We present the first study of baryon-baryon interactions in the continuum limit of lattice QCD,
finding unexpectedly large lattice artifacts. Specifically, we determine the binding energy of …

Over the last decade, numerical solutions of Quantum Chromodynamics (QCD) using the
technique of lattice QCD have developed to a point where they are beginning to connect …

Loosely-bound objects such as light nuclei are copiously produced in proton-proton and
nuclear collisions at the Large Hadron Collider (LHC), despite the fact that typical energy …

The quantization condition for two-particle systems with an arbitrary number of two-body
open coupled channels, spin, momentum, and masses in a finite volume with either periodic …

The binding energies of a range of nuclei and hypernuclei with atomic number A≤ 4 and
strangeness| s|≤ 2, including the deuteron, dineutron, H-dibaryon, He 3, He Λ 3, He 4, He Λ …

The flavor-singlet H dibaryon, which has strangeness-2 and baryon number 2, is studied by
the approach recently developed for the baryon-baryon interactions in lattice QCD. The …