I. Introduction
Strangeness degree of freedom opens a new dimension to our evolving picture of nuclei and also to our understanding of quark confinement in hadrons. Hyperons are baryons involving -quark(s) and hypernuclei are nuclei with embedded hyperon(s). Extensive strangeness physics programs have started with the advent of high-intensity hadron beams at J-PARC, Japan. A new E42 experiment [1] aims at searching for a six-quark dihyperon state, called H-dibaryon, in reaction.